Up and down conversion systems for production of emitted light from various energy sources including radio frequency, microwave energy and magnetic induction sources for upconversion

ABSTRACT

Methods and systems for producing a change in a medium. A first method and system (1) place in a vicinity of the medium at least one upconverter including a gas for plasma ignition, with the upconverter being configured, upon exposure to initiation energy, to generate light for emission into the medium, and (2) apply the initiation energy from an energy source including the first wavelength λ1 to the medium, wherein the emitted light directly or indirectly produces the change in the medium. A second method and system (1) place in a vicinity of the medium an agent receptive to microwave radiation or radiofrequency radiation, and (2) apply as an initiation energy the microwave radiation or radiofrequency radiation by which the agent directly or indirectly generates emitted light in the infrared, visible, or ultraviolet range to produce at least one of physical and biological changes in the medium.

CROSS REFERENCE TO RELATED APPLICATIONS

This application is a Continuation of U.S. Ser. No. 14/688,687, filedApr. 16, 2015, now allowed, which is a Divisional of U.S. Ser. No.12/943,787 filed Nov. 10, 2010, now U.S. Pat. No. 9,232,618, is relatedto Provisional Applications Ser. No. 60/954,263, filed Aug. 6, 2007, and61/030,437, filed Feb. 21, 2008, and U.S. application Ser. No.12/059,484, filed Mar. 31, 2008, the entire contents of each of whichare hereby incorporated herein by reference. This application is alsorelated to U.S. application Ser. No. 11/935,655, filed Nov. 6, 2007; andProvisional Applications Ser. No. 61/042,561, filed Apr. 4, 2008;61/035,559, filed Mar. 11, 2008, and 61/080,140, filed Jul. 11, 2008,the entire contents of which are hereby incorporated herein byreference. This application is related to U.S. patent application Ser.No. 12/401,478 filed Mar. 10, 2009, the entire contents of which arehereby incorporated herein by reference. This application is related toU.S. patent application Ser. No. 11/935,655, filed Nov. 6, 2007, andSer. No. 12/059,484, filed Mar. 31, 2008; U.S. patent application Ser.No. 12/389,946, filed Feb. 20, 2009; U.S. patent application Ser. No.12/417,779, filed Apr. 3, 2009, the entire contents of which are herebyincorporated by reference. This application is related to U.S.provisional patent application 61/161,328, filed Mar. 18, 2009, theentire content of which is hereby incorporated by reference. Thisapplication is related to U.S. provisional patent application Ser. No.12/417,779, filed Apr. 3, 2009, the entire content of which is herebyincorporated by reference. This application is related to PCTapplication PCT/US2009/050514, filed Jul. 14, 2009, the entire contentof which is hereby incorporated by reference. This application isrelated to U.S. patent application Ser. No. 12/725,108, filed Mar. 16,2010, the entire content of which is hereby incorporated by reference.

This application is related to and claims priority under 35 U.S.C. 119to U.S. provisional patent application 61/259,940, filed Nov. 10, 2009,the entire content of which is hereby incorporated by reference.

BACKGROUND OF THE INVENTION Field of Invention

The invention relates to methods and systems for producing light fromlower energy activation sources. The invention also relates to systemsand methods for broad band up conversion from the microwave and RFregime to electromagnetic radiation of higher photonic energy in the UV,VIS, and IR regime.

Discussion of the Background

Presently, light (i.e., electromagnetic radiation from the radiofrequency through the visible to the X-ray wavelength range) is used ina number of industrial, communication, electronic, and pharmaceuticalprocesses. Light in the infrared and visible range is typicallygenerated from an electrical energy source which for example eitherheats a material to extremely high temperatures where black bodyemission occurs (as in an incandescent lamp). Light in the visible andultraviolet range is typically generated by heating a gas to anelectrical discharge where transitions from one electronic state of thegas atom or molecule occur with the emission of light. There are alsosemiconductor based light sources (as in light emitting diodes andsemiconducting lasers) where electrons/holes in a material recombine toproduce light emission.

Visible light is defined as the electromagnetic radiation withwavelengths between 380 nm and 750 nm. In general, electromagneticradiation including light is generated by the acceleration anddeceleration or changes in movement (vibration) of electrically chargedparticles, such as parts of molecules (or adjacent atoms) with highthermal energy, or electrons in atoms (or molecules). Both processesplay a role in the glowing filament of incandescent lamps, whereas thelatter process (electrons within atoms) occurs in fluorescent lamps.

The duality nature of light (or more generally electromagneticradiation) is such that light is both a wave (characterized by awavelength and amplitude) and a discrete parcel of energy or photon(characterized by its frequency times the Planck constant (denoted ℏ).The higher the frequency the higher the quantized energy carried by theradiation. All energy above the visible is considered in manycircumstances to be ionizing radiation as its photons carry sufficientenergy to ionize matter.

For reference purposes, infra-red (IR) radiation just beyond the red endof the visible region; and, ultra-violet (UV) radiation has a shorterwavelength than violet light. The UV portion of the spectrum is dividedinto three regions: UVA (315-400 nm), UVB (280-315 nm) and UVC (100-280nm).

Industrial lamps used in lighting applications cover the visible rangeof wavelengths for proper white perception. Thermal sources like heatedfilaments can be made of different type conductors, includingW-filaments, halogen-protected W-filaments, and electrically inducedhigh temperature plasmas (arc lamps).

The power (energy emitted per second) of a radiant source is frequentlyexpressed in watts (W), but light can also be expressed in lumens (lm)to account for the varying sensitivity of the eye to differentwavelengths of light. The derived relevant units are the radiance(luminance) of a source in W/m² (lm/m²) in a certain direction persteradian (unit of solid angle) and the irradiance (illuminance) of asurface in W/m² (lm/m² or lux).

With the development of ultraviolet sources, ultraviolet radiation isbeing increasingly utilized for industrial, chemical, and pharmaceuticalpurposes. For example, UV light is known to sterilize media and is knownto drive a number of photo-activated chemical processes such as thecross-linking of polymers in adhesives or coatings. Typically,ultraviolet sources use gas discharge lamps to generate emitted light inthe ultraviolet range. The emitted light is then optically filtered toremove many of not all of the non-ultraviolet frequencies. Ultravioletlight can also be produced in semiconductor phosphors from theexcitation of these phosphors from high energy sources such as, forexample, X-ray irradiation.

With the development of infrared radiation sources, infrared radiationis being increasingly utilized for communications and signalingpurposes. Typically, infrared sources use broad spectrum light sourcesreferred to as glowbars to generate a broad spectrum of light centeredin the infrared range or use lasers to emit very specific infraredwavelengths. For the broad band sources, the emitted light is opticallyfiltered to remove many if not all of the non-infrared frequencies.

It is generally desirable to have devices, materials, and capabilitiesto convert light from one frequency range to another. Down conversionhas been one way to convert higher energy light to lower energy, as usedin the phosphors noted above. Up conversion has also been shown wherelower energy light is converted to higher energy light. Typically, thisprocess is a multi-photon absorption process where two or more photonsare used to promote an excited electronic state in a host medium whichin turn radiates at a wavelength of light that has a higher energy thanthe energy of the incident light which promoted the multi-photonabsorption process. Both down conversion and up conversion have beenstudied and documented in the past.

Up conversion and down conversion of electromagnetic radiations are veryrelevant to various industrials fields. Photo-activated chemicalreactions find broad use in the industry from catalyzing reactions toBio-modulation of therapeutic agents. However, UV radiation suffers froma lack of depth of penetration in matter especially biological media,polymers and most solids). For this reason, UV based photo-initiation islimited by direct line of site which prevents volumetric applications.

UV has been limited to reactions taking place on the outer surfaces ofmaterials may they be solids or liquids; organic or inorganic;biological organs, living tissues and composites thereof, structuralcomposites, materials residing inside chemical tanks/reactors for foodprocessing or hydrocarbon chains fractionation (to name a few examples).

Recently, there has been interest in the development of microcavityplasma devices which have been shown to have robust lightingcapabilities. These devices are unitarily connected devices driven by acommon electrode shared between the microcavities patterned on a commonsubstrate. Lamps have been made from arrays of microcavity plasmadevices including dielectric barrier structures in each of themicrocavoties. The microcavities have used diamond-shaped cross sectionsand anodized aluminum for the dielectric barriers. The microcavityplasma devices require no ballast. In addition, the microcavity plasmadevices have operated at pressures up to one atmosphere and beyond,thereby minimizing or eliminating the pressure differential across thelamp packaging.

Yet, the fact that these devices are unitarily connected devices drivenby a common electrode shared between the microcavities patterned on acommon substrate restrict utilization of the microcavity devices todiscrete device applications such as lamps and recently have been usedin transistor structures.

SUMMARY OF THE INVENTION

In one embodiment, there is provided a method for producing a change ina medium. The method (1) places in a vicinity of the medium at least oneupconverter including a gas for plasma ignition. The upconverter isconfigured, upon exposure to initiation energy, to generate light foremission into the medium. The method (2) applies the initiation energyfrom an energy source including the first wavelength λ₁ to the medium,wherein the emitted light directly or indirectly produces the change inthe medium.

In one embodiment of the invention, there is provided a method forcuring of a radiation-curable medium. The method applies initiationenergy throughout a composition comprising 1) an uncuredradiation-curable medium and 2) at least one upconverter including a gasfor ignition and configured, upon exposure to the initiation energy, togenerate light for emission into the medium. The light is of awavelength to cure the uncured medium by polymerization of polymers inthe medium. The method cures the radiation-curable medium by activatinga photoinitiator in the radiation-curable medium.

In one embodiment of the invention, there is provided a method forproducing a change in a medium. The method (1) places in a vicinity ofthe medium an agent receptive to microwave radiation or radiofrequencyradiation, and (2) applies as an initiation energy the microwaveradiation or radiofrequency radiation by which the agent directly orindirectly generates emitted light in the infrared, visible, orultraviolet range to produce at least one of physical and biologicalchanges in the medium.

In one embodiment of the invention, there is provided a system forgenerating light. The system included a low frequency energy sourcewhich radiates a first wavelength λ₁ of radiation and a receptor havinga microscopic dimension and which receives the first wavelength λ₁ ofradiation and generates a second wavelength λ₂ of the emitted light inthe infrared visible or the ultraviolet wavelength range.

In one embodiment of the invention, there is provided a microwave or rfreceptor. The receptor includes a free-standing ionizable-gascontainment filled with an ionizable gas which upon receipt of firstwavelength λ₁ of microwave or rf energy emits light in the visible orultraviolet wavelength range.

In one embodiment of the invention, there is provided a microwave or rfreceptor. The receptor includes a partitioned structure including atleast two reaction components and includes a partition separating the atleast two reaction components, whereby mixing of the two reactioncomponents upon microwave or rf radiation at first wavelength λ₁produces at least one of a chemiluminescent or bioluminescent reactionfor emission of the second wavelength λ₂.

In one embodiment of the invention, there is provided a method forproducing light within the body of a subject. The method places insidethe body a gas containment sealed with an ionizable gas, irradiates thebody with microwave or if energy, and ignites a plasma in the gas of thegas containment to thereby produce light within the body of the subject.

In one embodiment of the invention, there is provided a system fortreating or diagnosing a human or animal subject. The system includes agas containment sealed with an ionizable gas. The gas containment isconfigured to be disposed inside the human or animal subject. The systemincludes a source of microwave or rf energy configured to broadcast themicrowave or if energy into the human or animal subject. The source ofmicrowave or rf energy at least partially having the capability togenerate a plasma in the gas of the gas containment to thereby producelight within the body of the human or animal subject.

It is to be understood that both the foregoing general description ofthe invention and the following detailed description are exemplary, butare not restrictive of the invention.

BRIEF DESCRIPTION OF THE FIGURES

A more complete appreciation of the invention and many of the attendantadvantages thereof will be readily obtained as the same becomes betterunderstood by reference to the following detailed description whenconsidered in connection with the accompanying drawings, wherein:

FIG. 1A is a schematic depicting a system according to anotherembodiment of the invention in which the initiation energy source isdirected to a medium having energy modulation agents disbursed withinthe medium;

FIG. 1B is a schematic depicting a system according to anotherembodiment of the invention in which the initiation energy source isdirected to a container enclosing a medium having energy modulationagents disbursed within the medium;

FIG. 1C is a schematic depicting a system according to anotherembodiment of the invention in which the initiation energy source isdirected to a container enclosing a medium having energy modulationagents segregated within the medium; and

FIG. 1D is a schematic depicting a system according to anotherembodiment of the invention in which the initiation energy source isdirected to a container enclosing a medium having energy modulationagents segregated within the medium in a fluidized bed configuration;

FIG. 2 shows that the UV emission induced by a nitrogen and a heliumplasma are different;

FIG. 3 show that the UV and VIS emissions from the low-pressuremercury-argon discharge;

FIG. 4 shows emission lines from a nitrogen/hydrogen plasma covering theUVA target range;

FIG. 5 is a schematic of a wet etch pattern illustrating theundercutting that takes place under the resist (the etching is downwardand sideways);

FIG. 6A is a schematic of a dry etch pattern (resulting in well definedtrenches);

FIG. 6B is a schematic depicting carbon-carbon bonds forming a saturatedsurface on a wall 39 of one of the UCC structures;

FIG. 7 is a schematic showing how after removal of the patterningresist, the starting wafer can be capped with a flat quartz wafer (forexample) to form gas containers;

FIG. 8A is a schematic showing how after removal of resist, two mirrorimaged wafers (using a wet etch) are mated to form the gas containers;

FIG. 8B is a schematic showing how after removal of resist, two mirrorimaged wafers (using a dry etch) are mated to form the gas containers;

FIG. 9 is a process schematic showing the release layer being removed,followed by patterning;

FIG. 10 is a process schematic showing two versions of the gascontainers of the invention made using the large scale repeatable andreproducible processes;

FIG. 11 is a schematic showing different shapes of the gas containersdepending on how the starting wafer is capped and how the trenches areformed;

FIG. 12 is a process schematic showing the filling of the gas containerswith the appropriate gases prior to sealing;

FIG. 13 is a schematic showing the internal wall of the glass containersbeing surface modified using Li and/or Na;

FIG. 14 is a schematic showing the production of the gas containerscarried our using standard semiconductor processes where over 100,000 upgas container converters can be made per 150 mm wafer;

FIG. 15 is a schematic showing metal traces deposited through patterningand sputtering to position electrical pads that would be negativelybiased for the subsequent placement of carbon-nano-tubes (CNTs) throughfluidic self assembly;

FIG. 16 is a schematic showing CNTs attached using a metallizationprocess (e.g., sputtering);

FIG. 17 is a schematic showing that the shape of the up converters canbe controlled and showing that spherical or elongated shapes can bemanufactured in a reproducible manner;

FIG. 18 is a schematic showing that the shape of the up converters canbe further engineered for maximizing UV output and collimation to bedirected to an agent in the medium of the upconverting container;

FIG. 19 is a schematic showing a novel method for producing single anddouble metallic shell coatings not using wet chemistries;

FIG. 20 is a schematic of a double metallic shell that is applicable tothe gas containers of the invention as well as solid state crystallinesolids used for down or upconverters;

FIG. 21 is a schematic of a silicon tetrahedral building block of allsilicates [Si⁴⁺ (red) and O²⁻ (blue)];

FIG. 22 is a schematic representation of amorphous SiO₂;

FIG. 23 is schematic representation of amorphous silicate where aluminum(Al) is substituted for some Si to produce a charge deficiency;

FIG. 24 is schematic representation of the metastable equilibrium ofvarious alkali and alkaline earth metals around non-bridging oxygen;

FIG. 25 is schematic representation of showing the complexities of acaged substituted silicate structure;

FIG. 26 is schematic representation of zeolites composed ofalumino-silcate structures;

FIG. 27 is schematic representation of an Alkali-Alumino-Silicatenano-particle containing nano-pores (or silicate cages);

FIG. 28 is schematic representation of an alumino silicate nano-particlecoated with nano-diamond film or diamond like carbon or highlyconductive graphene material;

FIG. 29 is schematic representation of a nano-particle coated with anorganic film (for possible bioluminescence;

FIG. 30 is schematic representation of a partially coated to fullycoated Sodium-Alumino-Silicate particles the coating illustrated with Aufor plasmonics generation;

FIG. 31 is schematic representation of a carbon-Nano-Tube (CNT);

FIG. 32 is schematic representation of a microwave construction with anelectromagnet for testing gas emissions;

FIG. 33 is schematic representation of a microwave construction fortesting nano-particles for emissions after they have been filled withgas and sealed (no external gases);

FIG. 34 is a micrograph of iron oxide nanoparticles;

FIG. 35 is micrograph of conducto spheres;

FIG. 36 is schematic of direct irradiation in a biological media;

FIG. 37 is schematic of coaxial irradiation in a biological media;

FIG. 38 is schematic of the effects of RF stray fields in a biologicalmedia;

FIG. 39 is schematic of the effects of RF stray fields in a biologicalmedia;

FIG. 40 is schematic overview of other Broad Band FrequencyUp-Conversion Methods and Materials through Gas Reaction which shows twonano-particles necked together through an interface material to form amultichamber gas reactor;

FIG. 41 is a schematic depicting a general water glass composition;

FIG. 42 is schematic of another nano-particle structure (a tri-chambergas reactor);

FIG. 43 is schematic of a light wave propagation in different media;

FIG. 44 is schematic of a Φ-wave propagation in different media;

FIG. 45 is schematic of a multi-layer dielectric lens;

FIG. 46 is schematic of a Φ-wave propagating through a multi-layerdielectric lens;

FIG. 47 is schematic of luciferin and luciferase;

FIG. 48 is schematic of an encapsulated structure of the invention forbioluminescence;

FIG. 49A is a schematic of a multi-turn solenoidal coil showing theprojection of the magnetic field along the longitudinal axis;

FIG. 49B is a schematic of another multi-turn solenoidal coil showingthe projection of the magnetic field along the longitudinal axis;

FIG. 50 is a schematic of bird cage coil showing the projection of themagnetic field in a radial direction;

FIG. 51A is a schematic of a MRI arrangement suitable for the inventionand representative of a typical commercial MRI system;

FIG. 51B is a schematic of providing more operational detail to the MRIarrangement shown in FIG. 59A;

FIG. 52 is a schematic of a UCC structure including a capsule-typeregion for holding an upconverting gas and a down converting media;

FIG. 53 is a schematic of a UCC structure including a capsule-typeregion for holding an upconverting gas and a down converting media wherean activatable agent is attached thereto;

FIGS. 54-1A to 54-11 are a group of schematics depicting various processfor depositing a magnetic membrane structure or coating according to oneembodiment of the invention;

FIG. 55 is a side view schematic depicting up converters of oneembodiment of the invention having magnetic layers contained therein;

FIG. 56 is a side view schematic showing magnetically loaded containershaving single coating or double coating for plasmonic resonance effects;

FIG. 57 a top view schematic showing up converters of one embodiment ofthe invention having magnetic layers contained therein;

FIG. 58 is schematic of an RF plate capacitor configuration;

FIG. 59 is a schematic of an RF stray field applicator configuration;

FIG. 60 is a schematic description of a staggered RF stray fieldapplicator configuration;

FIG. 61 is a schematic description of a hybrid RF applicator whereadjustable electrodes are illustrated;

FIG. 62 is a schematic description of a staggered cylindrical RFapplicator configuration;

FIG. 63 is a schematic description of a cylindrically configuredstaggered cylindrical RF applicator is presented;

FIG. 64 is a schematic description of a cylindrically configuredstaggered cylindrical RF applicator configuration;

FIG. 65 is a schematic of a phased RF applicator capable of deliveringdifferent frequencies;

FIGS. 66A, 66B and 66C are schematics of different sets of solenoidcoils in different configurations designed to excite and stimulaterotational movements of para-magnetic gases and magnetic dipolescontained in various UCC structures of the invention;

FIG. 67 is schematic of a configuration for a serialized operation offour coil magnets that can operate out of phase;

FIG. 68 is a schematic depicting the operation of paired solenoids tocreate a re-entrant magnetic field path, where the paired solenoids areoperated in a serialized manner and/or out of phase between the pairs

FIG. 69 is a schematic of two electromagnetic coils working inconjunction with one another to form a reentrant magnetic field whichcan penetrate an object when the field emanates from one coil to theother;

FIG. 70A is a schematic depicting a number of electromagnets disposedaround a work piece or a patient where the magnetic field paths areconfigurable;

FIG. 70B is a schematic of a magnetic configuration illustrated foraligning and strengthening the magnetic field;

FIG. 71 is a schematic depicting the utilization of variable fieldstrength multipath-way magnets, the size of which can be made large tohost a patient or small to be used for localized treatment on a patient;

FIG. 72 is an illustration of a large multipath way magnet used inconjunction with a reentrant electromagnet;

FIGS. 73A and 73B are schematics of various sets of solenoid coils eacharranged in a configuration to treat local parts of an object or apatient;

FIG. 73C is a schematic showing four magnetic coils spaced apart to hosta patient and operate in series for the purpose of a targetedpenetration into a work piece or patient and for the triggering of aplasma in the UCC structures of the invention;

FIG. 74 is a schematic of a temperature, electric field, and magneticfield probe all of which can be measured simultaneously;

FIGS. 75A and 75B are schematics of sensors (including temperature,magnetic and electric field strengths) employable in various embodimentsof the invention;

FIG. 76 is a schematic of an area array of sensors provided under andabove a patient or a work piece to collect information and resolution ofthe field special distribution;

FIG. 77 is a schematic of the utilization of magnetic induction systemif a patient requires treatment in a limb and not an internal organ;

FIG. 78A is a photographic depiction of a phased array of dipoleantennas surrounding a phantom;

FIG. 78B is a schematic of a catheter of the invention having a gascontainer upconverter at or near the distal end of the catheter; and

FIGS. 79A and 79B are schematic representations of the in-vitro assaysand results thereof, where cells were exposed, through a phantom tomimic in-vivo penetration of the activation energy.

DETAILED DESCRIPTION OF THE INVENTION

The invention is directed to methods and systems for producingelectromagnetic radiation having desirable frequency windows (at leastone frequency within a desirable frequency range) from otherelectromagnetic radiation having lower or higher frequency ranges usingup converting transitional media or down converting transitional mediaas the case may apply. In various embodiments of the invention, theproduced electromagnetic radiation is then be used to activate an agentin a vicinity of the medium where the up converting transitional mediaor the down converting transitional media are disposed. In variousembodiments, the applied energy is considered to be up converted, as thephoton energy carried by radiation 1 has an energy level equal to hν₁(the product of Planck constant and frequency 1) is converted to ahigher energy hν₂, where hν₁ is less than hν₂. In various embodiments,the applied energy is considered to be down converted, as energy at hν₁,is converted to a lower energy hν₂, where hν₁ is greater than hν₂.

In various embodiments of the invention, there are provided systems andmethods for broad band up conversion from the microwave and RF regime toelectromagnetic radiation of higher photonic energy in the UV, VIS, andIR regime. The invention can encompasses a variety of applications wherethe up and down conversions are conducted inside biological media,inside human and animal bodies, and in chemical reactors to name but afew.

The present inventors have realized in particular that such upconversionprocessing can be used in various materials, chemical, medical,pharmaceutical, or industrial processing. The ultraviolet, visible,and/or near infrared light can then be used to drive photoactivatablereactions in the host medium.

Reference will now be made in detail to a number of embodiments of theinvention, examples of which are illustrated in the accompanyingdrawings, in which like reference characters refer to correspondingelements.

As shown in FIG. 1A, an exemplary system according to one embodiment ofthe invention may have an initiation energy source 1 directed at medium4. Activatable agents 2 and energy modulation agents 3 are dispersedthroughout the medium 4. The initiation energy source 1 may additionallybe connected via a network 8 to a computer system 5 capable of directingthe delivery of the initiation energy. In various embodiments, theenergy modulation agents 3 are up converters or down converters such asfor example fluorescent particles and other luminescent agents discussedbelow. In various embodiments, the energy modulation agents 3 are gascontaining up converter structures where energy from microwave radiationor radiofrequency radiation directly or indirectly generates emittedlight in the infrared, visible, or ultraviolet range to produce physicaland/or biological changes in the medium. As used herein, the term“change in the medium” includes but is not limited to the inducement ofa photoactivated reaction such as for example drug activation, cell orbacteria or virus or yeast kill, radical generation, sterilization,polymerization, hardening, curing, localized heating from the emittedlight, etc. One example of a biological change thus includes the thermalactivation or the photo-activation of therapeutic agent that in turntriggers a response in the cell viability in the medium.

In various embodiments, the energy modulation agents 3 are encapsulatedenergy modulation agents 6, depicted in FIG. 9A as silica encased energymodulation agents. As shown in FIG. 1A, initiation energy 7 (e.g. in theform of radiation from the initiation energy source 1) permeatesthroughout the medium 4. In some cases, the initiation energy 7 from theinitiation energy source 1 may only permeate partially through themedium. The initiation energy 7 can be completely or partially consumedin the conversion process. Both the initiation and induced radiation (oremission) can represent energy coupled to the medium during theirradiation process.

As discussed below in more detail, the initiation energy source 1 can bean external energy source or an energy source located at least partiallyin the medium 4. As discussed below in more detail, activatable agents 2and/or the energy modulation agents 3 can have plasmonics agents whichenhance either the applied energy or the energy emitted from the energymodulation agents 3 so as to directly or indirectly produce a change inthe medium.

In various embodiments, the initiation energy source 1 may be a linearaccelerator equipped with image guided computer-control capability todeliver a precisely calibrated beam of radiation to a pre-selectedcoordinate. In these embodiments, down conversion can be used togenerate internal light inside the medium. In these embodiments, x-raysor high energy particles from these or other sources can be used todirectly or indirectly trigger ionization in a gas containing upconverter structure of the invention. One example of such linearaccelerators is the SmartBeam™ IMRT (intensity modulated radiationtherapy) system from Varian medical systems (Varian Medical Systems,Inc., Palo Alto, Calif.). In other embodiments, the initiation energysource 1 may be commercially available components of X-ray machines ornon-medical X-ray machines. X-ray machines that produce from 10 to 150keV X-rays are readily available in the marketplace. For instance, theGeneral Electric Definium series or the Siemens MULTIX series are buttwo examples of typical X-ray machines designed for the medicalindustry, while the Eagle Pack series from Smith Detection is an exampleof a non-medical X-ray machine. As such, the invention is capable ofperforming its desired function when used in conjunction with commercialX-ray equipment.

In other embodiments, the initiation energy source 1 can be a radiofrequency or microwave source or infrared source emittingelectromagnetic waves at a frequency which permeates at least a part ofthe medium and which triggers or produces or enhances secondary radiantenergy emission within the medium by interaction with the energymodulation elements 6 therein, for example the gas containing upconverter structures of the invention. In other embodiments, theinitiation energy source 1 can be an ultraviolet, visible, near infrared(NIR) or infrared (IR) emitter emitting at a frequency which permeatesat least a part of the medium 4 and which triggers or produces secondaryradiant energy emission within medium 4 by interaction with the energymodulation elements 6 therein.

FIG. 1B is a schematic depicting another system according to anotherembodiment of the invention in which the initiation energy source 1 ofFIG. 1A is directed to energy modulation elements 6 placed in thevicinity of a fluid medium 4 (e.g., a liquid or other fluid-like medium)and held inside a container 9. As shown in FIG. 1B, the modulationelements 6 by their positioning in the medium have the mediumsurrounding the modulation elements 6. The modulation elements 6 areinside the medium and therefore intimately in a vicinity of the mediumto be activated thereabout each modulation element 6.

The container 9 is made of a material that is “transparent” to theinitiation energy 7. For example, plastic, quartz, glass, or aluminumcontainers would be sufficiently transparent to X-rays, while plastic orquartz or glass containers would be transparent to microwave or radiofrequency radiation. The energy modulation elements 6 (e.g., the gascontaining up converter structures) can be dispersed uniformlythroughout the medium or may be segregated in distinct parts of themedium or further separated physically from the medium by encapsulationstructures 10, as described below. As shown in FIG. 1C, theencapsulation structures 10 are separated from the medium, and yet arein a vicinity of the medium to be activated. A supply 11 provides themedium 4 to the container 9.

Accordingly, as used herein, “in a vicinity of” refers to theupconverters of the invention, such as for example the modulationelements 6 or the encapsulation structures 10 (e.g., the gas containingup converter structures) being disposed completely inside a medium,partly inside or partly outside a medium, adjacent a medium, orcompletely outside a medium where light from the upconverters irradiatesa part or the whole of the medium.

Alternatively, as shown in FIG. 1C, energy modulation agents such as thegas containing up converter structures of the invention and/or otherluminescent materials could be present in the medium in encapsulatedstructures 10. In one embodiment, the encapsulated structures 10 arealigned with an orientation in line with the external initiation energysource 1. In this configuration, each of the encapsulated structures 10has itself a “line-of-sight” to the external initiation energy source 1shown in FIG. 9C without being occluded by other of the encapsulatedstructures 10. In other embodiments, the encapsulated structures 10 arenot so aligned in that direction, but could be aligned perpendicular tothe direction shown in FIG. 9C, or could be randomly placed. Indeed,supply of fluid medium 4 could itself be used to agitate theencapsulated structures 10 and mix the fluid medium 4 inside container9.

FIG. 1D is a schematic depicting a system according to anotherembodiment of the invention in which the initiation energy source isdirected a container enclosing a medium having energy modulation agentssegregated within the medium in a fluidized bed 20 configurations. Thefluidized bed 20 includes the encapsulated structures 10 in aconfiguration where a fluid to be treated is passed between theencapsulated structures 10. The encapsulated structures 10 can includeboth energy modulation agents such as the gas containing up converterstructures of the invention and/or other luminescent materials and/orplasmonics agents as described herein.

In the either configuration of FIGS. 1C and 1D, the medium to be treatedin one embodiment would flow by the encapsulated structures 10, or flowalong with encapsulated structures 6, and the separation distancebetween the encapsulated structures 6, 10 would be set a distancesmaller than the UV penetration depth in the medium. Thus, as shown inFIGS. 1C and 1D, the medium being treated need not be stationary inorder for the encapsulated structures 6, 10 to be in a vicinity of themedium to be treated. In other embodiments, the medium to be treatedcould be stationary.

In further embodiments of the invention, robotic manipulation devicesmay also be included in the systems of FIGS. 1A, 1B, 1C, and 1D for thepurpose of delivering and dispersing the energy modulation elements 6 inmedium 4 or for the purpose of removing old product and introducing newproduct for treatment into the system.

A suitable initiation source (such as one of microwave sources or radiofrequency sources for up conversion) can be used to stimulate lightemission in the encapsulated structures 10. In one embodiment of theinvention described here, the concentration of light emitters in themedium or the spacing between the encapsulated structures 10 is set suchthat light emitters are separated from each other in the medium by lessthan a UV depth of penetration into the medium. Higher concentrationsare certainly usable and will generate higher UV fluxes should theenergy source have enough intensity to “light” all the luminescentparticles.

For a relatively unclouded aqueous medium, UV-B irradiance decreases to1% after penetration into the water samples between 0.2 m and 1 m,whereas UV-A penetrates on the order of several meters. For suchmediums, the concentration of light emitter is more determined by thetime needed for the intended UV flux to produce deactivation oractivation of an agent in the medium, rather than having to be set basedon a concentration of light emitter where the medium itself does notocclude the UV stimulated emission from penetrating throughout themedium. The placement of the light emitter in the vicinity of the mediumis not restricted by the optical density of the medium.

Accordingly, the upconverter structures of the invention (as discussedabove) can be provided on the interior of sealed quartz or glass tubesor can be provided coated on the surface of spheres or tubes, andfurther encapsulated with a silicate or another passivation layer. Inone embodiment, the gas containing up converter structures of theinvention are complexed with the X-ray down converting particles orother energy modulation agents permitting for example X-ray irradiationto also assist in this process.

Broad Band Up Conversion (BUC)

The following embodiments pertain to broad band up conversion (BUC)which converts a low frequency electromagnetic wave (in the microwave orRF regime) to a higher frequency electromagnetic wave (in the IR, VIS,or UV regime) using nano-scale material gas-containing composites.

Upconverting composite (UCC) structures of this embodiment of theinvention include gas and gas mixtures contained in capsules ofcontainers having at least one of their dimensions in the followingranges (e.g., 10 cm or 10 mm, 10 microns, 100 nm to 10 nm) that arehollow or porous. In the case of a nano-porous media, the gas iscontained inside a nano-particle which, in one embodiment, hasnano-pores. The morphology of such particles can be spherical (orsubstantially spherical). Other non-spherical morphologies may also beused. The mechanism in this embodiment of the invention for upconversion occurs by creating plasmas through the ionization of suitablegas or gas mixtures within the UCC structures.

In other embodiments, the upconverting composite structures of theinvention can be millimeter(s) to micron(s) in size.

Plasma is often referred to as the 4th state of matter and naturallyoccurs when gases are exposed to high intensity electric fields ofsufficient magnitude to overcome the work function or theionization-potential of gases. Plasma is therefore the mixture of a verylarge number of neutral gas atoms (or molecules) and individual charged,energetic, meta-stable, and unstable species with complex interactionsoccurring between them. Plasma is in general difficult to create andsustain atmospheric pressures (with one exception being an electricalarc discharge). Stringent pressure and energy transfer conditionstypically need to be satisfied before plasma ignition and sustainmentcan be achieved. In conventional practice, plasma sources have beenwidely designed for various purposes from lighting applications tochemical vapor deposition.

In general, when a gas in a container, typically at low pressures, issubjected to enough energy to ionize the gas molecules (or atoms) suchthat a significant number of the gas molecules (or atoms) loose one ofmore of their valence shell electrons, a plasma can be generated andmaintained. Of relevance is the fact that a plasma load (the ionizedgas) requires a power transfer to maintain the ionized gas, as wallcollisions and recombination of electrons and ions in the gas phasecause a loss of ions from the plasma. In the industry, RF inductivecoils operating at 13.56 MHz and microwave energy in the 2.45 GHz rangehave been used to couple power into a plasma and maintain ionization.

From a practical stand point, a plasma can be treated as a conductorbecause of its large population of energetically charged particles (boththe negative charges (i.e.; electrons) and the positive charges (i.e.;ions)) with the plasma conductivity being defined by the charge densityand the electron mobility. An ionized gas includes on average an equalnumber of positive and negative charges. For most plasmas, the extent ofionization is small, typically only 1 charge particle per 700 to 10,000neutral atoms or molecules.

The negative charge carriers are mostly electrons. Energy transfer(loss) from electrons is inefficient. Thus, electrons attain high energy(e.g., 2-50 eV). This permits high-temperature type of reactions (whichmake free radicals) in a low temperature neutral gas to occur. Theelectron energy is channeled into inelastic electron-neutral collisionswhich supply new charge species to the plasma and which generate lightemission.

In one embodiment of the invention, a plasma in one of the UCC structurebecomes the light source to trigger the activation of agents in themedium surrounding the UCC structures.

In one embodiment of the invention, in the presence of a static magneticfield, a charged particle resonates around magnetic lines of force at aparticular frequency, known as its rotation of cyclotron frequency. Thecyclotron frequency at which an electron enters the ECR is given as:ωce=q*B/mWhile in the static magnetic field, if the particle is subjected to atime varying electric field with a frequency equal to the cyclotronfrequency of the particle, and if the electric field is perpendicular tothe magnetic field (or at least has a component that is perpendicular tothe electric field), then the charge will absorb the energy of theelectric field quite effectively. This occurrence is widely referred toas ECR.

It is known that the gyrating electrons assume a helical path about themagnetic field lines. For a microwave frequency of 2.45 GHz, therequired B field strength for ECR is 875 Gauss (assuming and providedthe electric field is perpendicular to the magnetic field). Electronsthat enter the precession are referred to as “hot-electrons,” and theirkinetic energy is transferred to the valence electrons of the dischargegas. This energy transfer can be done after single or multiplecollisions). The plasma formed can be sustainable or unsustainable. Adischarge can be sustained when the loss mechanism (diffusion andrecombination) are balanced by ionization in a steady state. An ECRplasma is usually conducted at low pressures in the mTorr region. Powerabsorption takes place even if the excitations of the electric field areoutside of the ECR frequency. This is known as joule or collision orOhmic heating and can take place at high pressure (e.g., 100 mTorr orhigher).

Inductively coupled plasmas which operate in the RF regime are typicallyoperated at 13.56 MHz or 27 MHz. The frequencies are not restricted byany fundamental law of nature, but rather set to a frequency band clearof other radio communications. Microwave-generated plasmas can beoperated over a broad range from above 300 MHz all the way to 100 GHz,although the spectrum accessed is only this frequencies supplied fromcommercially available sources.

In one embodiment of the invention, the gases in the UCC structures havea low work function (or ionization potential). In its simplestdefinition, ionization is the ability of a photon to detach at least oneelectron from an atom or molecule. Furthermore, the ionization of asubstance depends on the energy of individual photons, and not on theirnumber.

UV radiation has very low penetration depth and resonates with theelectrons involved in covalent bonding between adjacent atoms. X-rayradiation is deeply penetrating and resonates with tightly boundelectrons (the inner core electrons) and induces transitions betweenallowable electronic energy states. X-rays and gamma rays (due to thehigher characteristic photon energy) can excite electrons and can ionizealmost any molecule or atom. Far ultraviolet light can ionize many atomsand molecules (a well known mechanism and well studied detrimentaleffect on living cells).

Across the electromagnetic spectrum, the spectral ranges and energystates depend on the frequency and the matter exposed to the radiation.Near UV, visible light, IR, microwaves and radio waves are in generalconsidered non-ionizing radiation. In other words, ionization(especially in solids) is not generally produced by radiation withwavelengths longer than 200 nm.

In general, low frequency radiation in the RF and microwave regimecouples energy through free rotation of molecules or the dipolarpolarization of parts of molecules (side groups). IR couples with thevibration of molecules, the optical through UV couples to the outerelectronic states of atoms and molecules. Soft X-ray and X-rays couplewith core electronic states of atoms and gamma rays couples with nuclearstates. Upon light generation from a source, the emitted spectrum of theradiant energy can be broad, or it can have well defined lines atcertain wavelengths (depending of the mechanism responsible for theradiation processes).

In one embodiment of the invention, gases of a particular polarity(molecular charge asymmetry) are chosen as the coupling media toimplement the upconverting process. Gases benefit from a high degree ofrotational freedom as compared to other molecules (whose mobility ishindered through their bondage to a network). Furthermore, gasestypically have a low ionization potential, as compared to crystallinesolids. In this embodiment, the chemical composition of the UCCstructures is selected not only to contain gas and gas mixtures but alsoto permit microwave coupling and UV or VIS transmission (for secondarylight emission), and/or to be compatible with metallization processes,and/or to be amenable to surface treatments which may functionalize thesurface for solvation, conjugation and other effects.

It is well established that the ratio of Na to Al in silicatesdetermines the short range order/structure of these materials, and hencethe silicate cages left within them. Other material chemistries (notcontaining sodium) are also suitable in different embodiments of theinvention to contain desirable gas and gas mixtures. In someembodiments, the UCC structures include ionization-assisting materialsattached to increase microwave coupling efficiency and thereforefacilitate the ionization process of the gas mixtures associated withthe UCC. Ionization-assisting materials can possess high electronmobility and density; these materials include carbon-nano-tubes (CNTs)and graphene amongst others. These attached or associated materialswould serve as electron pumps (as it is well established that microwavecouples to CNTs and graphene through electrical conductivity).

Microwaves are electromagnetic waves whose frequencies range from 300MHz (Megahertz) to 300 GHz (Gigahertz). Their corresponding wavelengthsrange from one meter to sub-millimeters. The lower end of the microwaveregion borders radio frequencies, while the upper end is adjacent toinfrared frequencies. Microwaves are widely used in modern society.

Microwave radiation obeys the laws of electromagnetism according to thewell known Maxwell's equations (which are the four basic laws ofelectromagnetism). When a material is exposed to microwave energy, thefollowing set of equations can be used to characterize theelectromagnetic properties:

-   -   Conductive materials (Ohm's law): J=σE (where σ is the        conductivity of the material).    -   Dielectric materials: D=εE where c is the permittivity of the        material which can also be written: c=ε₀k′ where ε₀ is the        permittivity of empty space and k′ is the dielectric constant of        the material.    -   Magnetic materials: B=μH where μ is the permeability of the        material which can also be written as μ=μ₀μ_(r) where μ₀ is the        permeability of empty space and μ_(r) is the relative        permeability of the material, where    -   D is the flux of the electric induction,    -   B is the magnetic flux density,    -   H is the magnetic field vector, and    -   J is the conduction current density.

In one upconversion embodiment, plasmas in the UCC structures arecreated through the ionization of suitable gas or gas mixtures withinthe UCC. In one embodiment of the invention, the attachment of a CNTmaterial and graphene can facilitate the plasma ignition and plasmasustainment while the UCC is exposed to microwave and/or radio frequencyRF radiation. This process can be facilitated further by the presence ofa magnetic field applied with a proper orientation. The application ofMW and RF can be from a wide range of sources including magnetrons,Klystrons, Gyrtrons, Traveling Wave Tubes and Solid Sate Amplifiers andpossible a helix sustaining a strong alternating field such as those ininductive coupling.

The optimal microwave frequency will be application dependent. Theplasma generation process triggered by microwave ionization of gasesoccurs, in one embodiment, under the presence of a magnetic field havinga proper orientation vis-à-vis the RF/MW field (i.e., orthogonaldisposition). Once the gas in the UCC structure is ionized, electrons inthe plasma can be made to enter a precession movement. The magneticfield strength required to force precession of electrons is much lessthan that required for the precession of ions (due primarily to thedifference in mass between electron and ions). The magnetic fieldstrength can be therefore selected to resonate with electrons whilebypassing ions.

The added elastic collisions (due to induced precession movements)reduce the MW energy required for generating and maintaining the plasma.Higher MW frequencies typically results in higher disassociation ratesand lower electronic temperatures compared to lower RF/MW frequencies.Conversely, the higher the frequency of the incident microwave energythe less the penetration depth is. In one embodiment, as discussed inmore detail later, MRI equipment can be used in conjunction withmicrowave equipment for triggering plasma intensification, thereforetaking advantage of the well established equipment base in the field ofMRI.

The chemical properties of the UCC structures can be imparted throughsurface modifications, which can be tailored for specific applications.For example, the UCC surface can be coated with thin metallic coatingsand can be functionalized for attaching molecular structures that, inone embodiment, can undergo chemical changes after UV irradiation fromthe UCC structures. Various divers applications for the resultantupconverted light were discussed above and other applications arediscussed hereafter.

A metalized and/or functionalized UCC structure is referred to herein asa UCC-MF. A UCC-MF outputting in the UV is abbreviated herein asUCC-MF-UV. Molecular structures attached to the UCC-MF surfaces can be atag used for subsequent chemical tracing purposes, a catalyst forinitiating other chemical reactions, therapeutic agent for subsequentbio-modulation.

In one application pertaining to in-vivo photo-initiated modulation oftherapeutic agent, the upconverting composite would be mm, micron andnano meters. For reaching the nucleus the composite is made very small(nanometer scale) and can deeply penetrate inside biological tissue ofanimals or humans. More specifically, in this embodiment, the UCCstructure would be designed to diffuse and penetrate a cell or even topenetrate the nucleus of a cell of a specific organ or “the targetsite.”

In one application pertaining to in-vivo photo-initiated modulation oftherapeutic agent, the upconverting composite would be larger and placednearby or proximate the specific organ or “the target site.”

In one embodiment of the invention, when the UCC (perhaps with anattached therapeutic agent) is at a target site, a deeply penetrating MWradiation along with an applied magnetic field are used to ignite thegas mixture of the UCC. The gas mixture subsequently generates UV lightnecessary to modulate the therapeutic agent(s). One specific examplewould be for activation of psoralen.

Nano-UCC(s) have the potential to optimize psoralen excitation in vivo.The emission band tuning can be achieved through the UCC synthesis (gasmixtures and gas containment material selection) which would permitsensitization of the broad family of psoralen derivatives that can befabricated.

Other application areas could use gasses of different emissioncharacteristics. These applications could include: the sterilization ofsurrounding media, the photoactivation of resins in curing and bondingapplications, as well as to other application areas discussed above orbelow or known to be photoactivatable. In those applications, the knownemission characteristics of plasma gases are used to select which gasesto contain in the UCC structures.

The paper “Emission Characteristics of a Glow Discharge in a Mixture ofHeavy Inert Gases with Iodine Vapor,” by A. K. Shuaibov and I. A.Grabovaya. Uzhgorod National University, Uzhgorod, 88000 Ukraine, Opticsand Spectroscopy, Vol. 98, No. 4, 2005, pp. 510-513. Translated fromOptika i Spektroskopiya, Vol. 98, No. 4, 2005, pp. 558-561, the entirecontents of which are incorporated herein by reference, describes theemission characteristics of a low-pressure UV excimer-halogen lamppumped by a longitudinal DC glow discharge. In that paper, the dischargewas initiated in mixtures of heavy inert gases with iodine vapor at atotal pressure of 100-2000 Pa and with a power deposited into the plasmaof 10-100 W. Current-voltage characteristics of the glow discharge andemission spectra of the plasma in the region of 190-360 nm werereported. The radiation intensity at the resonance line of the iodineatom (206.2 nm) and the intensity at the peaks of the XeI(B-X) (253 nm)and I2(B-X) (342 nm) emission bands were analyzed as functions of thepressure and partial composition of the mixtures of Ar, Kr, and Xe withiodine vapor, as well as the electric power of the glow discharge.

In one embodiment of the invention, mixtures such as these can be usedin the UCC structures of the invention which, upon plasma generation,would emit similar emission lines. The light emission spectrum of theplasma can be controlled by adapting the gas composition.

The paper “Plasma technology: a solution for UV curing on 3-dimensionalsubstrates,” by Tunja Jung, Peter Simmendinger, Katia Studer, WolfgangTobisch, presented at: Radtech e|5: UV & EB Technology Conference 2006.(RadTech International, NA, Apr. 23-26, 2006, Lakeside Center atMcCormick Place Chicago, Ill.), the entire contents of which areincorporated herein by reference, describes that, by adapting processparameters such as the type of the gas, it is possible to emit UV lightbetween 200 and 380 nm. This paper described the use of these radiationsto induce photoinitiated polymerization. Arc-lamps were used for theUV-curing applications, with emissions not significantly different fromthe emissions of the plasma process described above. In this paper,during the plasma process, the light was emitted throughout the chamber.In other words, UV-plasma curing required placing the coated substratein the light source. As previously mentioned, in one embodiment of theinvention, the light emission spectrum of the plasma can be controlledby adapting the gas composition.

FIG. 2 (reproduced from that paper) shows that the UV emission inducedby a nitrogen and a helium plasma are different. Depending on thespectral photosensitivity of the UV-curable formulation, it is thereforenecessary to check whether the UV emission of the plasma overlaps theabsorption of the photoinitiator in the coating system. The emissionproperties of plasmas can be customized by modifying the gas contentsand pressure and thus can be adapted to specific technical applicationrequirements. The systems shown in FIGS. 32 and 33 (discussed below) canbe used to engineer the desired emission from the UCC structures beforeintroduction of the UCC structures into the target medium or site.

In another study published in the INSTITUTE OF PHYSICS PUBLISHINGJOURNAL OF PHYSICS D: APPLIED PHYSICS. J. Phys. D: Appl. Phys. 37 (2004)1630-1638 PII: S0022-3727(04)74779-8. entitled: “Relative enhancement ofnear-UV emission from a pulsed low-pressure mercury discharge lamp,using a rare gas mixture,” by S Kitsinelis, R Devonshire, M Jinno, K HLoo, D A Stone and R C Tozer, the entire contents of which areincorporated herein by reference. In this paper, the physical reasonsfor the enhancement of near-UV and visible emissions from a low-pressuremercury-argon discharge under pulse drive conditions are explained. FIG.3 (reproduced from that paper) shows the UV and VIS emissions from thelow-pressure mercury-argon discharge. A small admixture of Krypton asthe buffer gas leads to maximizing radiative emissions. The conditionsof operation that maximize the enhancement of near-UV and visibleradiation, including the effect of the buffer gas, are described. Thispaper describes that, for a pulsed discharge, electron-ion recombinationfollowed by cascade radiative transitions is the process responsible formost of the 365 nm emission and that argon with a small admixture ofkrypton (as the buffer gas composition) leads to maximum radiativeemission. The gases can be tuned though mixtures of proper ratios toemit at any frequency within UVA.

In one embodiment of the invention, mixtures such as these are used inthe UCC structures of the invention which upon plasma generation insideemit similar emission lines.

Ammonia and argon gasses are also of special interest. Ammonia has beenused to create MASERs due to its response to microwave energy. Itabsorbs microwave energy, and in various embodiments significantrotational energy can be pumped into ammonia molecules. Most gassesincluding argon can be ionized using microwave radiation and using aTesla coil or a combination thereof. These two gases can be used as abase from which other gases can be added to produce specific UV or VISor IR spectral emissions of interest. FIG. 4 shows emission lines from anitrogen/hydrogen plasma which would be expected to have similaremission lines.

In one embodiment of the invention, upconverting of low frequencyradiation (microwave or RF) into high frequencies uses non-solidemission media (i.e. the gases in the UCC structures). The advantages ofusing microwave reside in two main factors: a) the depth of penetrationof low frequency radiation far exceeds the penetration depth of IR andUV and b) the low frequency regime is inherently non-ionizing (lowenergy photons) and does not trigger adverse immune responses like inthe case of high intensity high dosage x-rays or gamma rays.

Examples of Broad Band UCC Structures of the Invention:

In one embodiment of the invention, a hollow gas-filled container (of arange on the order of millimeters to microns to sub-microns in aprinciple diameter) is designed to be deployed within an object ordispersed in a medium. In one example, the object can be a target organor tissue in a patient near a sight where for example a photosensitivechemotherapeutic agent (e.g., psoralen) has been localized. In oneexample, the medium can be a UV-activated resin or epoxy for joining twoobjects together, such as two semiconductor substrates or twosemiconductor die or two circuit board elements or a combination ofthese being joined. In one example, the object being treated can be acrack in a structural member such as a bridge structure or a highwaymember in which the crack has been pre-filled with the UV-activatedresin or epoxy This UCC “capsule” structure once in the target or mediumis exposed to a combination of microwave energy and/or high magneticfield in order to produce light (for example UV, VIS, or IR light or acombination thereof) from the plasma gas in the gas-filled container toactivate an agent in the medium such as for example a chemotherapeuticagent or a photoactivatable resin. In some applications, the generatedlight is used to sterilize or pasteurize the target medium, separatefrom or including using the generated light to activate achemotherapeutic agent or a photoactivatable resin.

In one embodiment of the invention, an applied magnetic field can rangein strength from 0.01 Tesla to 11 Tesla. In other embodiments, nomagnetic fields are applied. In other embodiments, higher magnetic fieldstrengths can be utilized. In one embodiment of the invention, themagnetic field can be substantially uniform and/or can be oriented alongthe axis of current-carrying coils producing the magnetic field. Such anaxis oriented along the axis of current-carrying coils will be referredto herein as a main magnetic axis. Such coils can be made ofsuperconductors, which in various embodiments can be cryogenicallycooled.

In one embodiment of the invention, the RF and/or microwave energy canvary from 13 kHz to 300 GHz with incident powers varying from about 1 Wto 10 kW. These RF and microwave sources can operate in a continuousmode or a pulsed mode with high peak powers and/or low duty cycles.Various RF and microwave devices, capable of either pulsed or CWoperation, are well known in the art, and devices generating this typesof pulsed or CW RF and/or microwave radiation are suitable for theinvention.

In one embodiment of the invention, the volume of the UCC capsulestructure can range broadly from the cubic nanometer scale to the cubiccentimeter scale. In the lower size scale, the volume of the gascontainer can range between 30,000 nm³ and 250,000 nm³ with wallthicknesses in the range of 10 to 100 Å. The UCC capsule structure canbe made even larger in volume, with larger wall thicknesses, for thesame purpose described above; i.e., for the purpose of containing a gasto be exposed to microwave and/or magnetic fields. In one embodiment ofthe invention, some of the walls of the UCC capsule structure can bemade thicker than others. In one embodiment of the invention, one wallis deliberately made very thin (as will be discussed in more detailbelow).

In one embodiment of the invention, the shape of the gas container inthe UCC capsule structure can also vary, without diminishing itsfunctionality; in many cases a sphere, cylinder, or ellipsoid is moresuited for microwave coupling and/or plasma generation. In oneembodiment of the invention, the shape of the walls can also enhance thestructural integrity of the container; e.g., spheres and ellipsoids tendto be structurally superior to prismatic shapes, ceteris paribus.

The gas containers described here, in one embodiment of the invention,are designed to be exposed to the combination of a strong magnetic fieldalong with pulses of electromagnetic fields.

In one embodiment of the invention, the magnetic gradients referred toabove are produced using coils located in different positions along theaxis of the strong magnetic field and the axis of these coils areoriented perpendicular to the axis of the strong and uniform magneticfield. The pulsed and short lived magnetic field gradients are thereforedesigned to be able to orient and reorient magnetic dipoles 90 and 180Efrom the central axis. FIGS. 49 and 50 (below) provide more details ofvarious magnetic field applicators.

In the absence of a material, the magnetic flux is expressed as B=μ₀ H,where H is called the magnetic field strength and μ₀ is a constantcalled the permeability of free space. Inserting a specimen into thecoil carrying a current (and hence having an axial magnetic field fluxB) does influence the magnetic field. Generally, the orbital and spinmagnetic moments within atoms respond to an applied magnetic field. Theflux lines are perturbed by the presence of the specimen. The resultantequation becomes expressed asB=μ ₀(H+M),where magnetization M is defined as the magnetic moment per unit volume.For a given material of volume V, the magnetization is therefore theratio of the magnetic moment divided by the volume:M=μ ₀ /V

Magnetic materials tend to concentrate flux lines. Examples magneticmaterials include materials containing high concentrations of magneticatoms such as iron, cobalt and nickel. On the other hand, diamagneticmaterials tend to repel flux lines weakly. Examples of diamagneticmaterials include water, protein, fat and other genetic materials.Magnetic susceptibility χ is expressed the ratio of:χ=M/HThe permittivity of diamagnetic materials is below 1. The permittivityfor Paramagnetic materials is above. The permittivity for ferromagnetic,ferromagnetic and anti-ferromagnetic materials is between 100 to1,000,000.

As for paramagnetic gases, applying a magnetic field would tend toorient the dipole moments. In other words, the gas attains amagnetization. With higher temperatures, however, the thermal energy k*Tmay exceed the torque alignment applied by the magnetic flux onto thegas dipoles.

In one embodiment of the invention, the energy recipe defined (i.e., thecombination of RF and/or microwave energy along with in some cases amagnetic field) for irradiation of the UCC structures includesparameters such as for example the magnitude and direction of the strongmagnetic field, the frequency, power, the electric field strength, themagnetic field strength, a direction of the RF/microwave coils thatproduce the gradients, and continuous vs. pulsed operation (with definedpeak powers and duty cycles). In one embodiment of the invention, theseenergy recipe parameters are computer controlled, as shown in FIG. 51(below).

Different energy recipes will likely be required for different UCCstructures or for different gas containers in the UCC structures or theUCC capsule structures. (Unless specifically set forth differently a UCCstructure will refer to any of the UCC capsule structures or the othergas containment structures discussed herein.) In one embodiment of theinvention, the energy recipe is designed to trigger ionization of gasesin the UCC structures. Once ionized, the gases enter a plasma phase ofmatter. In one embodiment of the invention, the plasma ignition need notbe sustained for a long period of time. If the chemo-therapeutic agentand the UCC are properly oriented and good energy transfer withminimized scattering; then, Plasma maintenance for even a microsecondcan generate substantial amounts of UV, VIS, or NIR light. If on theother hand UV light is not properly directed then more UV light isrequired to trigger the chemo-therapeutic agent.

In one embodiment of the invention, the UCC structures (filled withpreselected gasses or gas combinations) can emit in the UVA range uponplasma ignition. One especially suitable emission for chemotherapeutictreatment is emission at about 360 nm+/−50 nm. Accordingly, the gasesand gas mixtures are selected to work in conjunction with the gascontainer and the available energy recipes to produce the desired lightemission and the various examples here are provide solely forillustrative purposes.

In one embodiment of the invention, the walls of the UCC structures areUV transmissive so that the UV emissions from the interior gas (orgasses) pass from the inside of the gas container to the outside of thegas container with minimal losses due to absorption, scattering or othermechanisms. The size of the wall (and its absorption characteristics)will be a design consideration for the UCC structures. In one embodimentof the invention, the walls of the UCC structures are transmissive toX-rays or high energy electron beams which can be used to trigger plasmaignitions in the UCC structures of the invention. X-ray and RF can beapplied at the same time. X-ray radiation can be applied to the UCC. TheUC's inner walls can have a thin coating of a material able to interactwith X-ray photon to generate secondary electrons.

In one embodiment of the invention, the gas container material is beable to: withstand the electron temperatures during plasma ignition,withstand the pressure build up resulting from the temperature rise,permit both the magnetic field and the RF and microwave energy tointeract with gases while bypassing the walls of the container and/ortransfer a substantial part of the generated UV radiation to the outsideof the gas container. Any desirable frequency with the UVA can betriggered using the appropriate set of gases.

In one embodiment of the invention, gases such as Ne, Xe, He, Hg, H₂,N₂, Ar, Kr (or combinations thereof) can be used. For example, gasmixtures Ne+He, Ne+He+5% Xe, Ne+5-10% Xe can be used as well othercombinations and other mixture ratios. The percent Xe addition listedabove is by atomic percent. Hg+Ar emit at the 360 nm; Ne+1% Ar alsoemits at 365 nm. A small admixture of Krypton as the buffer gas can leadto radiative emission enhancements. Furthermore; other gas combinationscan be used, including iodine vapor with various impurities.

The properties of a plasma can be customized by modifying processparameters (magnetic field strength, microwave power and frequency) orimpurities of the reactive gases leading to plasma formation.

The range of pressure in the gas container can be between 0.01 and 100Torr. Other ranges considered more practical include a pressure between0.5 and 5 Torr. Though other pressures are suitable, the structuralintegrity of the gas containers may be best suited for this range of 0.5and 5 Torr based on theoretical calculations. The size and shape of thecontainer will partially determine the pressure range selected.Furthermore, the mean free path of the electrons decreases withincreasing pressures and vice-versa. Hence, at low pressures, sustainingplasma may be frustrated by electron diffusion and loss the interiorwall surfaces of the gas containers.

Alignment through a magnetic field (especially with 0.1 Tesla and abovemagnetic field strength) along with the ionization of the microwavefield, in one embodiment of the invention, provides one controlmechanism for energy conversion that is not typically available in theabsence of the magnetic field. Upon the RF/MW frequencies being tunedand applied orthogonal to an applied magnetic field, the electrons inthe plasmas in the UCC structures can enter an electron cyclotronresonance or can gain kinetic energy without entering ECR. In eithercase the plasma disassociation rate is enhanced in the presence of a Bfield regardless of its orientation. This is because various electronstravel on random trajectories once they are generated; so that, certainelectrons will find themselves in favorable trajectories to a gain andincrease in their kinetic energy. Under certain conditions of orthogonalB and E fields, the electrons can be confined to a circular trajectoryleading to their magnetically induced confinement.

The magnetic field forces the precession of the liberated electronswhich in turn collide with the various gases and impart further energy,permitting ionization and plasma maintenance. The presence of themagnetic field permits a lower overall externally imposedelectromagnetic energy to have to be used. The lowering of the totalenergy required to obtain UV output is very beneficial in view of thefact that the gas container may be disposed inside an animal or humantissue (in vivo or in vitro).

In one embodiment of the invention, the UCC structure can befunctionalized and attached to a drug delivery vehicle and sentthroughout the body to target tumor site. The UCC structure can play therole of a UV light source to trigger desirable reactions throughphoto-initiation. Photo-initiation is a known mechanism used in variousmedicinal, pharmaceutical and chemical reactions. In one embodiment ofthe invention, the photo initiation can be performed at 360 nm (+/−50nm) to trigger for example psoralen (and psoralen derivatives withbio-therapeutic functionality) inside a diseased cell or nucleus. Thebenefits of psoralen are known, but few techniques have been able toactivate psoralen inside a UV skin depth of a biological sample.

The energy required to trigger psoralen is in the range of about 2photons at 360 nm (+/−50 nm). In the 360 nm range, the followingcalculation illustrates one example of a suitable gas container gaseousmixture:

Chemical Electronic Energy per Energy per mole (J/mol) Energy Species &Emission photon (J) # particles per (kcal/mole) Gas Mixtures λ = nm E =(h*C)/(λ) E (ev) mol = 6.02E+23 1 kcal = 4.18 kJ H₂ + N₂ 360 5.51799E−193.44E+00 3.32E+05 1.39E+03 (Plasma)Assuming a van der walls radius to 3 Angstroms (0.3 nm)

Effective Number of ionized to hν for hν for Atomic Capsule particlesneutral atoms 360 nm 360 nm Radius nm volume nm³ inside Volume 1:700energy (J) energy eV 0.3 49,244 164,148 23.450 5.51799E−19 3.44E+00Energy Output Charging time Number of Output efficiency Capsule of thecapsule, eV in one second excitations per sec (UV transmission) OutputeV 8.08E+01 l.00E+04 8.08E+05 0.75 6.06E+06If one assumes that the ionized to neutral atom ratio is close to1:10,000 then the energy output of the capsule is calculated to be 4.24H 10⁵ eV.

In one embodiment of the invention, to improve the efficiency of thecoupling energy and to minimize scattering a protrusion can be designedonto the gas container to facilitate the attachment of the drug and tocollimate and maximize the UV delivery with minimal scattering

In one embodiment of the invention, the gas container can be coated witha metal coating such as a Au or Ag coating through vapor deposition orthrough wet chemistry. The metal coating permits plasmonic effects whichenhance the light output of the capsule (and possibly alter its outputfrequency).

In one embodiment of the invention, the interior wall of the gascontainer can be treated with plasma or wet chemistry to facilitate theionization of the gases, prior to filling and sealing the gascontainers. Gas mixtures can be chosen to have an affinity for oneanother to lower the work function and facilitate plasma ignition.

For various embodiments of the invention, the container can be undernegative pressure below atmospheric pressure and down to the mTorrpressure range. A hollow nano-meter size container can be filled withgases which emit in the UV The gas container can be fused silicastructure, a micro-balloon or a porous ceramic The container can be UVtransmissive. Quartz is reported to be around 75% transmission in theUVA range, and represents one material suitable for the invention.

Various methods can be used to produce gas containers in various sizesranging from the centimeter range to the nanometer range. In oneembodiment of the invention, nano-meter size containers can be madethrough the various techniques described below. For the purposes ofterminology in describing such a method, a starting wafer is defined asthe wafer upon which the various patterning, etching, metal vapordeposition, bonding, gas filling, sealing, surface modification and allother processing steps intended for building the UCC structures of theinvention.

Construction of the UCC Structures of the Invention

One way to build the UCC structures would be to form the containervolume through suitable etching recipes, and then seal the startingwafer using another wafer to cap the volume formed therein. In thisexample, the gas container may have rounded parts (due to etching), anda substantially planar wafer can be used as a sealant wafer.

More complex methods can be used to build these and other gascontainers. Such steps can include: forming suitable groves and patternson two different starting silicate wafers and then aligning and matingthese wafers with the appropriate “hollowed out” features to form thegas container. The sealing can be done by heat or can be done usingchemistries that allow silicates to bond at or near room temperature.

One important part of the fabrication of the of the gas containers isthe use of a structural wafer under the starting wafer. This structuralwafer acts as a fixture and holds the starting wafer using a releaselayer. Either wet etching or dry etching can be used to form desirableconcave features in the starting wafers. Wet etching can use for examplechemicals such as hydrofluoric acid, nitric acid, acetic acid.Typically, the isotropic etching pattern resulting from wet etching is adisadvantage in semiconductors; however, the undercutting that takesplace under the resist (i.e., the etching downward and sideways) isactually advantageous in this case since the undercutting permitsrounded edges to be formed. Also, since wet etching is isotropic, it canbe used to form patterns that are disposed in the plane of the startingwafer. In one embodiment of the invention, this procedure can produce aglass container with rounded internal walls.

FIG. 5 is a schematic of a wet etch pattern illustrating theundercutting that takes place under the resist to form the depictedconcave structures. This figure shows a carrier wafer 30 having arelease layer 32 and starting wafer 34 disposed thereon. A mask 35 isdeposited and thereafter has an opening defined thereon to expose thestarting wafer 32. A wet etch is used to generate the undercut portions36.

Plasma etching is anisotropic and leads to a trench definition havingmore rectangular edges than typically possible with wet etching. The useof RF generated plasmas coupled to RF power supplies is a known,effective, and efficient method suitable for the invention. Gaseousetchants such as fluorine and chlorine based gases can be used. Otheretching gasses include: BCl₃, Cl₂, CF₄, CHClF₂, CHF₃, CH₂F₂, CH₃F, C₂F₆,C₃F₈, C₄F₈, HBr, HCl, HF, NF₃, SiF₃, SiF₄, SF₆ or combinations thereof.Additives such as argon, oxygen, hydrogen, and nitrogen (which aretypically included between 1 and 10 ppm levels) can be added to theetching gas. The etching rate can be controlled using temperature andenergy. The rates of etching can be between 10 and 350 Angstroms permin. FIG. 6A is a schematic of a dry etch pattern (resulting in welldefined trenches). This figure shows a carrier wafer 30 having a releaselayer 32 and starting wafer 34 disposed thereon. A mask 34 is depositedand thereafter has an opening defined thereon to expose the startingwafer 32. A dry etch is used to generate the trench-like portions 38.This method using plasma etching to form the concave structures would beused when square sided walls are not considered an impediment for theUCC container.

Hydrogen additives increase selectivity toward etching SiO₂. Some ofhydrogen additives can influence the surface chemistry of the quartzwall left behind (called the side wall passivation or side wallprotection). This side wall blocking passivation forms when (forexample) the carbon atoms contained within the reactive etchant speciesmentioned above enter into chemical bonding with each others and formcarbon-carbon bonds resulting in a saturated surface. FIG. 6B shows aschematic depicting carbon-carbon bonds forming a saturated surface on awall 39 of one of the UCC structures. The carbon atoms from the sidewall protection layer on the side wall of the trenches may enter intothe plasma mix (when the glass containers are infused with the desirablegases and sealed) and possibly shift our UV emission output. On theother hand, in another embodiment of the invention, an oxide richsurface can be retained through an oxygen plasma burn to remove thecarbons prior to sealing the containers. The strong electronegativepotential of oxygen may lower the ionization potential of the gasessubsequently stored in the quartz container. Since dry etching isanisotropic, it can be used to form patterns that are disposed acrossthe surface of the starting wafer in any pattern defined by the mask onthe starting wafer. This can lead to a glass container with roundedinternal sidewalls. Regardless, the container can then be sealed fromthe top (as shown in FIG. 7 ) with a plate 40 to form a small scale cap(after the proper gases have been infused inside the nano-metercontainers).

The wall chemistry left behind after etching of the walls of the gascontainers may play an important role in the functionality of the gascontainers. The walls can have a surface energy that favors theionization of the gases contained within the containers. In other cases,the surface energy will be unfavorable to plasma ignition. The ionizedgases inside the glass containers would be repulsed, attracted by theelectrostatic forces residing on the surfaces of the walls. These may beimportant consideration in view of the small physical dimensionscontemplated in the invention.

In the case of dry etch chemistry, the sidewall protection filmdescribed above (which varies in thickness between 10-30 Å) is leftbehind from many etchant chemistries that are used. Accordingly, dryetching can be considered as a plasma treatment that can produce aninterior surface of the gas container that can range from an oxidizedsurface on one end of the spectrum to a polymerized surface at the otherend of the spectrum. As a plasma treatment, this treatment can occur asan additional step after wet chemistry is used to form the concavestructures. By ranking order, the chemistries that can be used and leadfrom oxidizing to polymerizing include NF₃, CF₄, CF₃Cl, CF₃Br, C₂F₆,CHF₃, C₃F₈, C₄F₁₀ and C₂F₄. On one side of the spectrum, the addition ofan oxidant is desirable (such as O₂). On the other side of the spectrumin order to consume the oxidants, H₂ can be used and is desirable insome cases.

Further surface modification of the walls of the gas containers can beperformed for other purposes that would be beneficial, such as forexample plasma formation, luminosity and mechanical integrity.

FIG. 7 is a schematic showing how after removal of the patterningresist, the starting wafer can be capped with the plate 40 (e.g., a flatquartz wafer) to form gas containers. Both wet and dry etching can beused. FIG. 8A is a schematic showing another embodiment of the inventionand depicting how after removal of resist, two mirror imaged wafers 42,44 (using a wet etch) are mated to form the gas containers. This methodis more complex but desirable. A more rounded container can be obtainedprior to removing the release layer. FIG. 8B is a schematic showing howafter removal of resist, two mirror imaged wafers 46, 48 (using a dryetch) are mated to form the gas containers.

FIG. 9 is a process schematic showing the release layer 32 having beenremoved, followed by (or proceeding) patterning at step 17-1, themasking and patterning at step 17-2, and the etching at step 17-3 torelease and separate the UCC structures from each other. In thisembodiment, a dry etch is used to obtain the gas containers. FIG. 10 isa process schematic showing two gas containers 50, 52 of the inventionmade using the large scale repeatable and reproducible processesdiscussed above.

FIG. 11 is a schematic showing different shaped gas containers dependingon how the starting wafer is capped and how the trenches are formed.FIG. 11 shows a half-spherical containment 54, a spherical containment56, a capped rectilinear containment 58, and mated rectilinearcontainment 60.

FIG. 12 is a process schematic showing the filling of the gas containers56, 60 with the appropriate gases prior to sealing. The gas containerscan be treated using HF to etch the edges. Gases such as Ne, Xe, He, Hg,H₂, N₂, Ar, Kr can be used as the fill gases. Also gas mixtures Ne+He,Ne+He+5% Xe, Ne+5-10% Xe can be used. The percent Xe addition is byatomic percent. Hg+Ar emit at the 360 nm; Ne+1% Ar also emits at 365 nm.Furthermore, other gas combinations can be used, including iodine vaporwith various impurities. After the gas fill, the gas containers can betreated to an HF bath solution to treat their edges to produce the UCCstructures 62, 64.

FIG. 13 is a schematic showing the wall 66 of glass containment 50 beingsurface modified on the interior using Li and/or Na interior surfacemoieties 68. In one embodiment of the invention, the internal wall ofthe gas containers can be surface modified by diffusing lithium andsodium into the silicate container. Both sodium and lithium arerelatively small ions. This treatment is best performed when the twohalves of the gas containers are still open. The diffusion of lithiumand sodium to the internal walls can increase the positive charges ofthe internal walls which would repulse a portion of the population ofpositively charged ions produced during the plasma ignition.Furthermore, if lithium and or sodium are leached out of the glass walland into the plasma, these ions can release significant light and hencetrigger more energy generation. Ion beam processes can be used to supplythe lithium and sodium ions onto the interior walls of the gascontainers of the invention. In these cases, an anneal stage is added toensure proper diffusion of the Li and Na ions. Sodium would lower theionization potential of gases and gas mixtures.

In one embodiment of the invention; the outer walls of the glasscontainer can be strengthened using external additives 70 such aspotassium. In one embodiment of the invention; potassium can be used tocreate compressive stresses that increase the structural integrity ofthe wall 66. The potassium surface modification of the outside walls isexpected to done after the containers have been sealed and released. Theoutside wall of the glass container of the invention can be strengthenedusing potassium diffusion. This technique can increase the strength ofthe gas container of the invention. The strength of the gas containerscan be thus engineered. In turn, the strengthening of the glasscontainers increases its structural integrity and permits the use of thegas filled containers at different pressures.

Once the two halves of the gas containers are mated and the gascontainers are sealed, a series of patterning and etching can be done torelease the gas containers, through deep and fast dry etching. Once thecontainers are singulated from the starting wafer, their surfaces can beetched (by time and temp in an HF bath) to reduce the wall thickness andround the edges. When the gas containers are subjected to an HFtreatment, the chemical strengthening using potassium diffusion is donesubsequently to the etching of their outer surfaces.

Regardless, FIG. 14 is a schematic showing the production of a pluralityof gas containers 72 carried our using standard semiconductor processeswhere over 100,000 gas container converters can be made per 150 mm wafer74.

In one embodiment of the invention, a metal coating such as Au or Ag forplasmonic activity can be applied at the wafer level using metal vapordeposition or can be applied through wet chemistry (after the gascontainers have been singulated). Prior to metal coating, a choice istypically made as whether or not to undergo the chemical strengtheningstep using potassium diffusion.

In one embodiment of the invention, various means can be used to createnano-porosity on the interior or exterior surface of the gas containersof the invention.

Further surface modification where by the gas containers (with orwithout down converters contained within) can have a dielectric layerand a metallic shell and possibly an additional protective layer. Thewet chemistry processes described before are applicable to the gascontainers. This final protective layer can be made of bio-compatiblechemistries that facilitate drug delivery within biological livingbodies.

In another embodiment of the invention, the gas containers are coatedwith a material having magnetic properties or to have anultra-nano-particle having magnetic properties (that fits within the gascontainer similar to the illustration provided in FIG. 53 .)

As noted earlier, a combination of microwave and strong magnetic fieldscan be used to ignite plasma and generate UV light. A well known sourceof magnetic field with all the desirable magnetic gradient and controlsis available in MRI machines with superconducting magnets enabling up to11 Tesla. In one embodiment of the invention, an applicator of RF and ormicrowave energy is provided having a proper applicator design, antenna,high frequency coil, and a mirror for quasi-optic. The microwave and RFapplicators that can be used in this invention include but are notlimited to waveguide applicators, direct microwave irradiation usingantennas, stray field applicators, capacitive parallel plates, coaxiallines, quasi-optical microwave devices, coils and solenoids and other RFand Microwave devices that can be derivatives of the fundamentalmicrowave and RF designs. Discussed below are schematic illustrations ofvarious microwave and RF hardware.

In one embodiment of the invention, the coils used for applying themagnetic gradient and all other modifications to the MRI machine areremovable, so that after the light therapy permitted in one applicationof the invention, the MRI machine can be returned to normal functionalstate. It is possible to use microwave designs that place the generatorsand power supplies outside the MRI machines to avoid any undesirableeffects caused through coupling of the magnetic field of the MRI withthe components and sub-systems of the microwave system. The microwaveenergy is then transmitted via an appropriate waveguide from thegenerator to the patient table.

In one embodiment of the invention, the waveguide passes through thewalls of the MRI main tunnel in which case special MRI equipment designshave be made to optimize the microwave energy delivery. This isespecially the case if microwaves using quasi-optical technologies(where a microwave beam is launched using a waveguide and reflected andfocused through a mirror to target a tumor area in the patient. Themicrowave applicators have to be made from non magnetic materials toavoid coupling to the magnetic field of the MRI. Aluminum and copperwaveguides and electrodes are therefore preferred

In one embodiment of the invention, an X-ray machine having a source, aprogrammable controller and radiation containment is used in conjunctionwith the MRI machine. Once the magnetic tracers (embedded in thesilicate containers encapsulating gases as well as a down convertingmedia) confirm that the therapeutic agents have been delivered totarget, the patient is subjected to an appropriate X-ray recipeconsisting of energy dose and pulse width.

Yet another embodiment of the invention is to combine suitable microwaveapplicators and X-ray hardware with MRI machines. Furthermore, highpower LASER sources in the IR regime can be used in MRI machines.

The various radiation energy sources can be used in combination or soloas the treatment may necessitate.

Examples of as Containers Having Carbon Nanotubes:

In one embodiment of the invention, the gas containers include carbonnano-tubes (CNTs) inside the UCC structures. In one embodiment of theinvention, a single-wall nano tube (SWNT) or a double-wall carbonnano-tube (DWNT) is attached to the internal or external wall of the gascontainer (preferably to the inside wall and preferably protrudinginside the volume of the gas container). The CNT structure facilitatesplasma ignition inside the gas containers.

The electronic properties of SWNTs are sensitive to the adsorption ofcertain gases. The charge transfer and gas-induced charge fluctuationare expected to significantly change the transport properties of theSWNT in the presence of an electric field. Furthermore, various gasmolecules adsorbed to SWNT can be either charge donors or acceptors tothe nano-tubes. Of special interest is the fact that NH₃, N₂, H₂, CH₄fall in the charge donor category, and thus can be used as gasses insidethe gas containers of the invention. O₂ for instance (which is notnecessarily used in this example) would act as a charge acceptors andwould make the nano-tubes p-type conductors.

In effect, the CNT not only can concentrate the electric field insidethe gas container but also can lower the ionization potential of gaseousspecies. The CNTs can be attached to the gas containers using a seriesof steps all of which are well established and practiced in thesemiconductor industry.

First, the desirable position of the CNT is defined, followed bypatterning, masking and metallization. FIG. 15 is a schematic showingmetal traces 76 deposited through patterning and sputtering to positionelectrical pads that would be negatively biased for subsequent placementof Carbon-Nano-Tubes 78 (through Fluidic Self Assembly). The metaltraces 76 would be formed for example of the underside of plate 40, suchthat when plate 40 is sealed to form the containments, theCarbon-Nano-Tubes 78 will be in place. The metallization can be doneusing various techniques including, evaporation, metal organic chemicalvapor deposition, and sputtering. One suitable method would besputtering. The sputtering process is widely used in semiconductors andcan be applied in this example to deposit metal traces of desirablegeometry along the surface of the starting wafer and/or in the concavecavities formed in the starting wafer surface.

Sputtering is based on simple principles. A vacuum chamber is filledwith argon gas. Plasma is struck and the argon ions are accelerated witha biasing voltage into the target material (Al or another metal ofchoice such as Au). Metal atoms are knocked off the target and land onthe wafers. Parameters such as pressure, bias voltage, generator andsputtering target can change the rate of deposition.

Au traces can be deposited from a Au coated sputtering target through apatterned mask onto the surface of the starting wafer and/or in theconcave cavities formed in the starting wafer surface. Al traces can bedeposited from an Al coated sputtering target. Cu traces can bedeposited from a Cu coated sputtering target. At least two metal traces(one on each side of the gas container) can branch out from the concavequartz starting wafer structure.

A quartz wafer plate 40 having the metal traces 76 is introduced in anon polar liquid bath and a negative bias is applied to the traces 76(through a pre-deposited common trace with an electrical pad on theperimeter of the wafer for applying the bias). The SWCNTs 78 arereleased in the non polar solution through a process similar to fluidicself assembly, known in the art. After settling and assuming thedesirable positions, the quartz wafer is elevated slowly to above thesurface of the non polar liquid (used for dipping). The wafer is thensubjected to a conformal coating to keep all the CNTs 78 in place. Forexample, another sputtering step is applied and the CNT are now fixed inthe designated groves. The mask would then be removed. Indeed, FIG. 16is a schematic showing CNTs 78 attached using a metallization process(e.g., sputtering). This method can yield a repeatable and reproducibleassembly from the nano to the micron scale. Upon removing thephoto-resist, the carbon nano tubes are held on place by virtue of themetal coatings. Besides CNTs, aluminum or copper filings or nanorods ornanoparticles can be added into the UCC structures.

With the CNTs in place, the gas containers are ready for gas filling andsubsequently sealing. Upon the quartz surface of the quartz startingwafer, a conformal coating of a silane adhesion promoter is dispensed.The silane adhesion promoter is designed for silica to open the Si—O—Simolecular bridge network on at least a near surface of the quartzwafers.

The sealing is performed by bringing the top wafer in close proximity toand aligned with the bottom wafer hosting the CNT 78 (in this case onlythe bottom wafer has CNT). The wafers are then sealed by having afixture that holds the wafers in close proximity under pressure forexample of 17 KN. This bonding can be done at or near room temperature.

The bonded wafers are then ready for another series of patterning andmasking steps to singulate and release the various gas containersthrough deep and fast dry etching. Once the containers are singulatedtheir surfaces can be etched (by time and temp in an HF bath) to reducethe wall thickness and round the edges (as described above). Thisfabrication process of forming the gas containers and releasing the gascontainers using standard lithographic patterning and other recognizedsemiconductor metal deposition and etching processes can occur with orwithout CNT inclusion.

FIG. 17 is a schematic showing that the shape of the UCC structures 62can be controlled and showing that spherical or elongated shapes can bemanufactured in a reproducible manner. FIG. 18 is a schematic showingthat the shape of the UCC structures 62 can be further engineered formaximizing UV output, and collimation to be directed to an agent in themedium of the up converting container can be realized. The UCCstructures 80 and 82 have respective longitudinal ends 84 and 86, wherelight from the ionized gas in the UCC structure will be directed orconcentrated. In other words, minimizing scattering and orienting thesolid angle output can be performed through controlling the shape of thewalls of the UCC structures.

Once the UCC structures are characterized in term of UV output; and, thesights of maximum UV output (or UV ports) have been identified, the UCCstructures can be further functionalized by adding biding agents to theUV ports (on the outer walls of the UCC). These binding agents are usedto fixate a chemical moiety such a psoralen in the proper conformationto the sight of maximum UV output in order to achieve photo-initiationof the chemo-therapeutic agent at the right site and with the leastnumber of UV photons. Furthermore, additional exposure of the psoralento UV radiation is designed to break the binder so that the psoralen isreleased (detached) from the UCC structure.

Examples of Double Metallic Coated Structures:

Sub-wavelength particles with metallic coatings exhibit very usefulproperties due to the local field enhancements created through opticalexcitations by the collective oscillation of the electrons, which arelocalized along the interface. A plasmonic phenomenon results in theconcentration of electromagnetic fields at the interface of the metaland the fluorescent crystalline material. This results in enhancedfluorescence and results in a frequency shift. The intensification andthe frequency shift depend on the dielectric, the fluorescence material,the size of the metalized particles, and the thickness of the coatingamong other parameters. The enhanced fluorescence that takes place ispredominantly occurring at the outer surfaces of the crystals.

Dual shell metallic coated fluorescent materials have gained interestrecently in view of the potential of added intensification, and in viewof other potentially useful inductive coupling between concentric metalshells.

In one embodiment of the invention, there is provided a method by whicha dual shell coating can be prepared. FIG. 19 is a schematic showing anovel method for producing single and double shell coatings. A plasmoniccoating 92 can be applied to a UCC structure 90 with or without CNT. Asecond coating 94 can further be applied to UCC structure 90 with orwithout CNT. Though the method is exemplified specifically for the gascontainer of the invention, the method is applicable to other metalizedsolid crystalline particles with plasmonic properties.

Similar to as before, a patterned wafer with electrical pads formedtherein is connected to a common ground plane using conventional vias.So that only the electrical pads are electrically conductive, the areasbetween the electrical pads are insulated using an organic or inorganicmaterial (such as SiO₂ or polymers). The patterned wafer is placedinside a liquid bath using a non polar liquid. The electrical pads areconnected to a negative bias creating a potential around the area of theelectrical pad.

The metalized glass containers (as described above but now freestanding) can be introduced into a solution of supersaturated solutionfor the purpose of partial hydrolysis of organo-metallic compounds. Thehydrolysis of TEOS and TMOS are well known and are used for the purposeof illustrating a simple method of creating a dual shell with highlyefficient semiconductor tools.

Starting with a metal alkoxides Si(OR)₄ where R is an alcohol radical,one can promote the hydrolysis and condensation. The hydrolysis can bepromoted by either an acid or base conditions. Acid catalyzed gels arepreferred in this case since these gels create chain like behavior intheir viscosity.

At one stage in the polymerization process, the gas containers withacidic functionalized attached can be passed on top of the non-polarliquid bath, with the wafer in a reversed biased condition. The glasscontainers would be electrostatically drawn to the electrical pads forthe wafer.

The wafer can be then elevated above the top surface and partiallydried. The wafer will then be taken to a CVD for depositing SiO₂ usingstandard silicate deposition processes. The top part of the gascontainers can be fully coated and the lateral sides can be partiallycoated.

The glass containers would therefore be coated partially (and not fullysince the glass containers lay on top of the electrodes). A second waferwith an adhesive but compliant release layer would be brought intoproximity and aligned with the wafer containing the gas containers. Thesecond wafer is then introduced to the CVD tool for depositing SiO₂ tocoat the top parts of the gas container and partially coat the lateralside of the glass container. CVD tools have the capability of wafertilting to optimize the coating uniformity.

The SiO₂ deposition recipe is designed to permit the formation of arelatively uniform SiO₂ coating since the top and bottom part get fullycoated (once) and the lateral parts get coated partially each time, butgo through the process twice.

The last step is metallization (as was described before); the sputteringprocess can be used effectively while the gas containers are held at thewafer level.

A dual shell metallization can therefore be synthesized using existingsemiconductor processes and can be arguably more repeatable andreproducible. FIG. 20 is a schematic showing how this novel methodproduces dual shell metallization on upconverter gas containers 96 or onsolid state crystalline doped up converters 98, as described in moredetail below.

Alternative Gas Containment Structures:

Silicates: FIG. 21 is a schematic of the fundamental silicon tetrahedralbuilding block of all silicates [Si⁴⁺ (red) and O²⁻ (blue)]. FIG. 22 isa schematic representation of amorphous SiO₂ network. FIG. 23 isschematic representation of amorphous silicate where aluminum (Al) issubstituted for some Si to produce a charge deficiency. The tetrahedralconfiguration formed is no longer electrically neutral, and some of thebridging oxygen sites become non-bridging oxygen sites. Theconcentration of non bridging oxygen increases in direct proportionalitythe Al³⁺ concentration. FIG. 24 is schematic representation of thissubstituted amorphous silicate structure further modified with ionicspecies. All these structures are suitable as UCC structures of theinvention.

In some glasses, to maintain charge neutrality (and avoid attractingvarious airborne polar molecules and gases) alkali and alkaline earthmetals (sodium, potassium, and calcium) are added to the silicatestructure. These ionic species break the silicate network and gettrapped in meta-stable equilibriums around non-bridging oxygen sites.These alkali ions become active in the microwave field (and can jumpover longer distances due to the wider and more spaced availablemeta-stable equilibrium sites).

FIG. 25 is schematic representation showing the complexities of a cagedsubstituted silicate structure. At the proper ratio of sodium toaluminum, large silicates cages are formed. At a molar ratio (Na/Al=1)the sodium alumino silicate glasses exhibit significant microwaveabsorption and diffusion. FIG. 24 is schematic representation ofzeolites composed of alumino-silcate structures. The crystallographicstructure of two zeolites formed by varying tetrahedras of (AlO₄) and(SiO₄) is shown. All these structures are suitable as UCC structures ofthe invention.

Unlike the previous example, charge neutrality is deliberately preventedand Zeolite exhibit useful properties as getter materials. Zeolites arewidely used as adsorbents. The tetrahedras result in unique structuresof special interest in the invention. Molecular sieves are manufacturedby crystallization from aluminum hydroxide, sodium hydroxide andwater-glass. In one embodiment, water glass can be used as a sealant forthe porous particles.

Under a crystallization process, the required sodium alumino-silicatestructure is formed. The formed zeolite crystals can be ion exchanged tofurther adjust the pore size. Molecules larger than the pore opening ofthe molecular sieve can not be adsorbed, smaller molecules can.Molecular polarity can be used to control/assist absorption. Gases withone degree of polarity may diffuse faster (e.g., ammonia is verysuitable for the diffusion process and microwave coupling).

It is possible to prepare phosphorous modified Zeolites/molecular sievesthrough an exchange process wherein a partially hydrogen, ammoniumexchanged sodium zeolite sieve is combined with H₃PO₄ and subsequentlytreated at elevated temperature and steam to react the proper siteleading to the obtainment of a zeolite with P₂O₅ in 2% to 5% by weight.The technology is described in U.S. Pat. No. 5,378,670 which referencedin its entirety in the invention. Various other catalysts that containphosphorous or phosphorous compounds can be used to derive phosphorouszeolites molecular sieves. These catalysts are described in variouspatents including U.S. Pat. Nos. 4,498,975; 4,504,382; 4,839, 319;4,970,185; and 5,110, 776. All these patents are hereby referenced intheir entirety.

FIG. 27 is schematic representation of an alkali-alumino-silicatenano-particle 90 in one embodiment of the invention containing thereinnano-pores (or silicate cages). These particles can be synthesized invarious ways, and some structures are commercially available underdifferent brand names. FIG. 28 is schematic representation of an aluminosilicate nano-particle 92 in one embodiment of the invention having acoating 94, such as for example coated with nano-diamond film or diamondlike carbon or highly conductive graphene material. FIG. 29 is schematicrepresentation of a nano-particle 97 in one embodiment of the inventioncoated with an organic film 99 (for possible bioluminescence). All thesestructures are suitable as UCC structures of the invention.

FIG. 30 is schematic representation of a partially coated to fullycoated sodium-alumino-silicate particles 100 in one embodiment of theinvention, the coating 102 is by way of illustration a metal coating(e.g., Au or Ag) for plasmonics generation. FIG. 30 shows the coating102 as a completely or partially encasing coating. FIG. 31 is schematicrepresentation of a carbon-nano-tube (CNT) 78 in one embodiment of theinvention, which can be attached to a porous or hollow nano-particle 100containing therein appropriate gas or gas mixtures. All these structuresare suitable as UCC structures of the invention.

A single or double wall CNTs can be used in any of the notedembodiments. As discussed earlier in the context of gas contained UCCstructures, CNTs are very receptive to microwave energy and can act asan electronic pump to stimulate the generation of plasma

As noted above, ammonia and argon are of special interest. Ammonia hasbeen used to create MASERs due to its response to microwave energy. Itabsorbs microwave energy, and in various embodiments significantrotational energy can be pumped into ammonia molecules. Argon can beionized using microwave radiation and a Tesla coil or a combinationthereof. These two gases can be used as a base from which other gasescan be added to produce specific UV or VIS or IR spectral emissions ofinterest. Commercially available silicate porous structures can befilled with the appropriate gases using a series of cycles of heattreatment under vacuum followed by back purge at elevated temperatures(this will assist the diffusion process). As discussed in relation toFIGS. 2-4 , a variety of gases can be used. The plasma generation can becarried out using microwave energy of various frequencies and magneticfield strengths.

The gases for diffusion are selected to have appropriate emissioncharacteristics for activation or treatment of agents in the mediumabout the UCC structures. FIG. 32 is schematic representation of amicrowave system 120 for producing pure-gas emissions from various UCCstructures of the invention. FIG. 32 shows a sealed tube 122 of reducedpressure extending through a microwave applicator 124. Different testgases can be introduced and optical emission data from plasmas of thosegases measured by the spectrometer. Once a particular gas having anappropriate emission wavelength is identified, the UCC structures can befilled with the candidate gas. FIG. 33 is schematic representation of amicrowave system 130 for comparison of different nano-particles foremissions (no external gases). Here, the gas-filled UCC structures areheld by rod 132 in the microwave applicator 134. Optical emission datafrom plasmas in the gas-filled UCC structures are measured by thespectrometer. This microwave system 134 permits one to readily compareemission spectra to that intended for a particular application.Furthermore, the microwave system of FIG. 33 represents schematically asystem for applying microwave energy (and optionally a magnetic field)to the UCC structures disposed in a medium placed inside the microwavesystem of FIG. 33 .

Various silicate structures can be utilized for the UCC structures ofthe invention.

Silica Gel: Silica gel including randomly linked spherical polymerizedsilicate particles are utilized in various embodiments of the invention.The properties of silica gels result from the size and state ofaggregation of the primary particles and their surface chemistry. Gelswith nearly 100% SiO₂ purity with tailor-made pore systems and surfaceproperties are used to “trap” the microwave-excitable gas inside.

For preparation, sulfuric acid and sodium silicate are mixed undercontrolled conditions to build the primary particles of the desiredsize, which polymerize and form the raw gel from which all types ofsilica gels are made. By controlling the washing, ageing, and dryingconditions, the physical parameters such as porosity (pore size anddistribution) and surface area can be adjusted to produce a range ofdifferent silica gel types. Silica gels are available in a wide range ofparticle sizes, each type having a well-defined particle sizedistribution.

Various chemical and thermal treatments can be used to improve thecharacteristics of silica gels as filter materials by controlling theirintenal surface areas and surface chmistries. These silica gels can beengineers to control their pore size and disctribution as well as theirinternal surface chmistries. The following patent application US2005/0205102 A1 is referenced in its entirety. The use of specialcatalysts and hydrothermal treatments is well documented in theliterature for example, Czarney et al, Przem. Chem. 46 (4), 203-207(1967) provide a study on pore structures following the varioushydro-treatments and catalysts.

Silica gel compositions containing alkali metals and alkali metal alloysare described in patent application US 2009/0041614 A1. The use ofSodium (Na), Potassiium (K), Rubidium (Rb) and Cesium (Cs). Sodium andPotassium (and their coumpounds) are preferred and are of specialinterest in the invention. Of particulat interset is the reportedreducing capability of the surface chemistry and how it reacts withSi—O—H groups to release hydrogen.

Precipitated Silicates: Precipitated silica include a three-dimensionalnetwork of coagulated primary silica particles. The latter grow to sizeshigher than 4-5 nm before they coagulate. Precipitated silicates aresynthesized by acidifying sodium silicate. Sulfuric acid is used as theacid source. A stirring vessel containing water is used, and theprecipitation is carried out under alkaline conditions. The choice ofagitation, duration of precipitation, the addition rate of reactants,their temperature and concentration, and pH can vary the properties ofthe silica. U.S. Pat. Nos. 4,422,880, 4,132,806, 4,015,996, and4,122,161 are referenced in their entirety.

Precipitated silicas distinguish from silica gels on the basis of porestructure. Precipitates typically have a broad meso/macroporous porestructure reflected in the pore size distribution, whereas gelsgenerally have a more narrow microporous or mesoporous structure.

These precipitated silicates once filed with a working gas are suitableas UCC structures of the invention.

Commercial products: VYCOR® glass code 7930 is an open-cell, porousglass which exhibits suitable absorbing properties for the invention.Due to its porosity, this material has an internal surface area ofapproximately 250 square meters per gram. This porous glass is widelyused in transistors, microminiature relays and other small devices. Ithas practical application in any sealed device that requires freedomfrom foreign contaminants. The open-cell network allows permeability ona selective basis—the species must be smaller than the microscopic poresto pass through the porous glass. The homogeneous pore diameters can becontrolled to average between 40 and 200 Angstroms. These commercialglasses once filed with a working gas are suitable as UCC structures ofthe invention.

Hollow Spheres (Cenospheres): Cenospheres are hollow spheres comprisedlargely of silica and alumina and filled with air and/or gases.Cenospheres are a naturally occurring by-product of the burning processat coal-fired power plants, and they have most of the same properties asmanufactured hollow-sphered products. The departure from all otherchemistries presented before is that cenospheres have Iron Oxide as partof their chemistry (Silica (55%-65%), Alumina (25%-35%), Iron Oxide(1%-5%), Titania (0.5%-1.5%)).

Size of theses hollow spheres are very large compared to what may beneeded in the biomedical application but spheres in the range of 10-350microns may find use in other applications not limited to extremelysmall sizes. FIG. 34 is micrograph of Iron Oxide nanoparticles. Thefollowing patent documents pertaining to cenospheres are incorporatedherein in their entirety by reference: U.S. Pat. Appl. Publ. No.20080190327 and U.S. Pat. No. 6,506,819.

These cenospheres once filed with a working gas can be suitable as UCCstructures of the invention through a gas diffusion process at elevatedtemperatures.

Conductospheres: Conductospheres are hollow glass microspheres coatedwith silver. These materials are typically incorporated into paints,adhesives and composites to provide these materials with electricalconductivity and to shield against electromagnetic interference (EMI)and radio frequency interference (RFI). Conductospheres are expected tobe microwave receptors in aggregate forms. FIG. 35 is micrograph ofConducto spheres.

Conducto spheres exist in various products. Product B-55 MicrosphereMaterial Base is an aluminosilicate in the range of 56 microns in medianparticle diameter and average Silver Thickness of 75 nm. Product M-18Microsphere Material Base is a hollow glass in the range of 19 micronsin median particle diameter and average Silver Thickness of 60 nm.

These conductospheres once filed with a working gas can be suitable asUCC structures of the invention through a gas diffusion process atelevated temperatures.

Alternative Hollow Spheres: Hollow Ni₃Si₂O₅(OH)₄ nanospheres can besynthesized via a facile deposition process at room temperature. Thedemonstrated diameters of the products is currently in the range of300-320 nm, and the average wall thickness is about 10 nm.

These hollow spheres once filed with a working gas can be suitable asUCC structures of the invention.

Receptor Structures:

In one embodiment of the invention, there is provided a system forgenerating light. The system includes a low frequency energy sourcewhich radiates a first wavelength λ₁ of radiation and includes areceptor having outside dimensions of millimeters or below and whichreceives the first wavelength λ₁ of radiation and generates a secondwavelength λ₂ of the emitted light in the infrared visible or theultraviolet wavelength range. The receptor in various embodiments canhave an outside dimension less than 1 cm, less than 1 mm, or less than 1micron.

The receptor in one embodiment can have microscopic dimensions. As usedin this context, microscopic refers to a dimensional scale on the orderof 900 microns or less, including nanometer size structures ranging insize from a few nm to 1000 nm. In one embodiment, the receptor hasmicroscopic dimensions are less than 400 nm so as to not representsignificant scattering centers for visible light. In one embodiment, thereceptor has microscopic dimensions are less than 50 nm so as to diffusethrough porous and semi permeable medium such as in living cells orbiological matter.

The receptor can include an ionizable-gas containment including anionizable gas. The receptor in one embodiment can be a free-standingmicrowave or if receptor, not attached to the circuitry delivering themicrowave or rf power to ionize the gas contained in the receptor. Thefree-standing microwave or rf receptor of this invention is configuredto be disposable in a medium nominally transparent to microwave or ifradiation and nominally opaque to UV or visible light. Accordingly, thewalls of the free-standing microwave or rf receptor of this inventionare nominally transparent to both microwave or if radiation andtransparent to UV or visible light.

The free-standing microwave or rf receptors of the invention thus differfrom plasma shells previously developed. For example, U.S. Pat. Appl.Publ. No. 2007/0132387 (the entire contents of which are incorporatedherein by reference) describes plasma shells encased between circuitryelements whose DC voltages produce plasmas inside the shells. Forexample, U.S. Pat. No. 7,604,523 (the entire contents of which areincorporated herein by reference) describe a number of techniques in theart and improvements thereon for forming plasma shells including thechoice of ionizable gas and the incorporation of secondary electronemitters. The techniques in U.S. Pat. No. 7,604,523 produce plasmashells with average diameters of about 1 mil to 20 mils (where one milequals 0.001 inch) or about 25 microns to 500 microns where 25.4 microns(micrometers) equals 1 mil or 0.001 inch. Plasma-shells can bemanufactured up to 80 mils or about 2000 microns in diameter or greater.The thickness of the wall of each hollow plasma-shell in U.S. Pat. No.7,604,523 is sufficient to retain the gas inside, but thin enough toallow passage of photons emitted by the gas discharge.

Accordingly, the techniques described in U.S. Pat. Appl. Publ. No.2007/0132387 and U.S. Pat. No. 7,604,523 for the formation of plasmashells including the surface treatments, the gas selection, and theincorporation of secondary electron emitters materials are suitable forthe formation of the free-standing microwave or if receptors of thisinvention, where the techniques applied there are selected to providewalls for the free-standing microwave or rf receptors of this inventionis nominally transparent to both microwave or if radiation andtransparent to UV or visible light.

The receptor can include a free space region within the containmentwhich upon ionization of the gas emits at least the second wavelengthλ₂. The ionizable-gas containment can have an outside dimension lessthan 1 cm, less than 1 mm, or less than 1 micron, less 100 nm, less than50 nm, or less than 20 nm. The ionizable-gas containment can be asilicate glass containing network formers (Aluminum, Lead, Phosphate)and modifiers (Sodium, Lithium, Calcium).

The ionizable-gas containment can be a porous structure permeable tomicrowave or if radiation. The porous structure can be at least one of asilicate glass, an alkali glass, a sodium glass, and a phosphate glass.The porous structure can be an ion-exchanged glass structure. The porousstructure can have an outside water glass to seal an ionizable gasinside.

The ionizable-gas containment can be at least one of a silica gel, aprecipitate silicate, a cenosphere, a conductosphere, or a hollowsphere. The ionizable-gas containment can be filed completely orpartially with at least one of hydrogen, argon, nitrogen, xenon,ammonia, iodine vapor; mercury vapor; an organic gas, andhydrogen-nitrogen mixtures, and mixtures thereof. In one embodiment,other low ionization materials such as sodium and barium strontium oxidecan be included inside the ionizable-gas containment. The ionizable-gascontainment can include a microwave or if coupler to promote electronemission into the free space region. The microwave or if coupler can beat least one of a carbon structure, a carbon nanotube, a single wallcarbon nanotube, a double wall carbon nanotube, grapheme, and metalmaterials or nanomaterials made of aluminum or copper.

The receptor can include a partitioned structure including at least tworeaction components and a partition separating the at least two reactioncomponents whereby mixing of the two reaction components upon microwaveradiation at first wavelength λ₁ produces at least one of achemiluminescent or bioluminescent reaction for emission of the secondwavelength λ₂. The reaction components can include bioluminescent orchemiluminescent reagents.

The partition cam be a microwave-activatable material which, uponactivation, opens the partition to mix the at least two reactioncomponents. The partition can be at least one of a microwave susceptiblematerial which heats upon microwave exposure, or a if susceptiblematerial which heats upon rf exposure, or a magnetic susceptiblematerial which is inductively moved upon exposure to a magneticinductive field. The partition can be material having a melting pointmaterial less than 30° C. The partitioned structure can be abiodissovable material. The partition can be a material having a meltingpoint greater than 30° C.

The receptor can be a structure including a shell and at least oneinterior void. This structure can be for example a cenosphere and aconductosphere. The interior void can be filled with at least one argon,neon, xenon, helium, ammonia, or an organic molecule.

The system for generating light includes a microwave or rf applicatorwhich directs radiation of the first wavelength λ₁ into an objectincluding the microwave receptor. The microwave or if applicator can beone of a waveguide applicator, a microwave or if antenna, or a microwavebeam source. The microwave beam source can be a focused beam sourceconcentration radiation of the first wavelength λ₁ into a region of theobject where the microwave receptors reside. The first wavelength λ₁radiation can be in a range of 1 KHz to 100 GHz.

The receptor can be configured to emit for the second wavelength λ₂radiation in a range from NIR to UV. The receptor can be configured toemit for the second wavelength λ₂ radiation which activates psoralen.The receptor can be configured to emit for the second wavelength λ₂radiation which photoactivates a resin material. The receptor can beconfigured to emit for the second wavelength λ₂ radiation which iscapable of sterilizing a medium in vicinity of the microwave receptor.The receptor can be configured to emit for the second wavelength λ₂radiation which photoactivates a photo-activatable adhesive connectingmembers together such as for example at least one of a semiconductordevice, a printed circuit board, or a semiconductor wafer. The receptorcan be configured to emit for the second wavelength λ₂ radiation whichphotoactivates photograftable materials. The receptors can be aplurality of receptors forming a fluidized bed for treating a fluidabout the receptors.

Viewed from a different perspective, the receptors can be consideredstructures for disposition in an homogeneous or inhomogeneous medium, ornearby an homogeneous or inhomogeneous medium, whose reception ofelectromagnetic field energy results in the production of emitted light.The receptors described above make use of materials and/or combinationof materials to assist in energy conversion inside a medium such as forexample a living body from one window of wavelengths and/or electricalfields of amplitudes and/or or currents flux densities to another windowof wavelengths.

In one embodiment, the flux density (electrical or magnetic or both)propagated in for example a polarizable biological media (e.g., anelemental volume inside the human body) induce in the materials and/orcombination of materials of the receptors a conversion of the incidentenergy into emitted energy which radiates from the receptors. Thisconversion may be more appropriately characterized in terms of thereactions of the materials and/or combination of materials of thereceptors with induced currents around the receptors especially at lowRF frequencies of 100 MHz and below. In this low frequency regime, ioniccurrents can take place, and these ionic current could in turn triggerbio-modulated responses.

Viewed from another perspective, the receptors can be consideredstructures for disposition in an homogeneous or inhomogeneous mediumwhose reception of electromagnetic field energy results in a receptorresponse. The receptor response can be as noted above the initiation ofa plasma contained in the receptor, the initiation of a bioluminescentor chemiluminescent reaction, the melting or dissolving of a member ofthe receptor, etc. The receptor response can be the triggering of amicroelectronic device included in the receptor. In which case, emittedlight may or may not be output from the receptor.

Microwave or RF Applicator Configurations:

For the purposes of illustration and to simplify discussion of the basicconcepts, incident wave propagation is considered along a z-axis of aCartesian coordinate reference system in the following description. Oneconsequence of Maxwell's equations is the self-propagation properties ofelectromagnetic waves. A time-varying magnetic field produces atime-varying electric field, which in turn creates a time-varyingmagnetic field. In a Cartesian reference system (x,y,z), with theassumption that propagation is along the z axis, both E and H aresinusoidally propagating along the z axis at the phase velocity of thewave.

The media to be treated in the invention can include various regionsacross which the incident microwave energy is going through to reach thedesired target site (tumor site for example). The incident wave goesthrough various absorption and reflections at each interface and variousmicrowave delivery methods are envisaged.

FIG. 36 is schematic of direct irradiation in a biological media. Asshown in FIG. 36 , the incident microwave will in all likelihood travelthrough different biological media (i.e., regions 1, 2, and 3) such asblood vessels and bone before arriving at the target medium (i.e.,region 4). This method can be used for example to deliver microwaveenergy to a tumor site but may not necessarily be appropriate for thedeliver of microwave energy to other target regions. In this directirradiation method of the invention, a microwave antenna can direct themicrowave energy, and a high intensity microwave power can be used topower the UCCs inside the tumor site at region 4.

FIG. 37 is schematic of coaxial irradiation in a biological media. Thisembodiment of the invention may result in tissue damage due to coaxinsertion to proximity of the tumor site. However, this embodimentavoids unnecessarily exposing regions 1, 2, and 3 to microwaveirradiation when delivering microwave energy to region 4.

FIG. 38 is schematic of the effects of RF stray fields in a biologicalmedia which results in tissue damage due to stray field probesinsertion. The stray field applicators can be powered with solid stateamplifiers and can be operated at low frequencies compared to microwaveapplicators (from 1 MHz to 400 MHz)

U.S. Pat. No. 5,187,409 (describing the HE 11 quasi-optic) isincorporated herein by reference in its entirety. The HE 11 is a quasioptical mode of propagation for microwave energy with specialorientation of the electric and field and magnetic field in the plane ofthe target. The divergent output of a waveguide is focused through aparabolic mirror to a minimal beam waist size close to one wavelength,which at 28 GHz is close to 10 mm. A highly concentrated beam can beobtained from a 28 GHz Gyrotron output. The peak power of this source is40 W per mm² and has been shown to ionize air. Such powers would bedetrimental to biological tissue, but could be acceptable for theirradiation of other media such as for example the above-noted resincuring applications. Of course, lower powers could be used forirradiating biological tissue.

In one embodiment of the invention, the microwave energy can propagateas if it were a focused light wave. Thus, biological tissue in regions1, 2, and 3 receive a lower level of microwave radiation exposure thanwhat would have occurred with the configuration depicted in FIG. 36 toobtain the same intensity of microwave energy in region 4. Otherquasioptical modes outputs are possible including TE02 and TE01;however, these modes do not have the same energy distribution and cannot as easily be focused using a mirror. The following patents areincorporated herein in their entirety by reference: U.S. Pat. Nos.3,010,088 and 3,188,588 which provide descriptions of these modes.

Gas Reaction Upconverter Structures

The upconverter structures in the embodiments below do not rely onplasma formation to generate light emission. Rather, in theseembodiments, an applied source of microwave, RF, magnetic induction, orultrasound energy reacts with the UCC structures to indirectly promotechemiluminescent or bioluminescent reactions. FIG. 39 is schematicoverview of other Broad Band Frequency Up-Conversion Methods andMaterials through Gas Reactions, dielectric lensing, multilayeredcomposites and organic Bioluminescence. FIG. 40 depicts a UCC structure150 having two compartment 152 and 154 separated by an interfacematerial 156. Each UCC structure compartment in one embodiment of theinvention contains a reactive component. Once the interface material 156is compromised, the two components undergo in one embodiment of theinvention an exothermic reaction and emit light during the reaction timeto for example bio-modulate therapeutic agent but not long enough toover heat the surrounding tissue. Molecules excited via oxidation chainreactions in the presence of catalysts can also be used. In otherapplications, the emitted light from the UCC structure 150 activatesphoto-activatable agents about the medium of the UCC structures. Theinterface material 156 can be a water glass (2Na₂O.SiO₂) which canprovide a build-in time delay prior to dissolution.

An example of a water glass composition can be as follows: Na₂O (17 to18%), SiO₂ (36 to 38%) and Iron Dioxide (0.05%). FIG. 41 is a schematicdepicting a general water glass composition.

The interface material 156 in one embodiment of the invention can be amagnetic material such that magnetic induction ruptures the interfacematerial. Such magnetic sheets or film compositions could be made ofFe—Si—Al flakes on a polymeric membrane with low melting points andengineered to have excellent permeability and magnetic absorption.

However, other magnetic film materials can be used such as BaFe_(10.5)Mn_(1.5) O₁₉ thin films. These films can be deposited by AlternatingTarget Laser Ablation Deposition (ATLAD) of BaFe₂O₄, Fe₂O₃, MnFe₂O₄Targets. The technique is well documented in IEEE transactions onMagnetics, Vol 44, No 11, November 2008 p-2966-2969 authored by Anton L.Geiler et al, the entire contents of which are incorporated herein byreference. The following patent is incorporated herein in its entiretyby reference: U.S. Pat. No. 5,483,037.

In a similar fashion, a triple component capsule structure could be madefor more reactive gas reactions (or chain reactions). FIG. 42 isschematic of another UCC structure 160 of the invention having multiplecompartments 162, 164, 166.

The UCC structures shown in FIGS. 41 and 42 could be made with thelithographic patterning and processes described above. For the sake ofillustration, the structures shown in FIGS. 41 and 42 could be viewed asa top-view of patterned concavities in starting wafer 34, where the wetor dry chemistries described above (along with proper masking) is usedto form these structures. Deposition and patterning can be used todeposit the interface material between the separate cavities.

For example, an interface material made of a polymer loaded withgraphite powder would be particularly susceptible to absorbing microwaveor RF energy and heat. For example, an interface material made of apolymer loaded with magnetic powder would be particularly susceptible tobeing ruptured upon exposure to an induction field. For example, aninterface material made of a polymer of different viscoelasticproperties than the silica wall would be particularly susceptible tobeing ruptured upon exposure to ultrasounds.

The cavities can be selectively masked and filled with their respectivereactive components.

Dielectric Lensing: A visible light propagating at the speed of lightslows down when it enter a glass. The speed of light inside glasses isreduced yet there no energy transfer. This is because in glasses thewavelength of a propagating wave is smaller than in free space. Theindex of refraction is the ratio of the speed of light in free space toinside the glass (n>1). In the visible, the index of refraction ofmetals nears infinity. FIG. 43 is schematic of light wave propagation indifferent media.

In the visible, one considers the index of refraction. There isequivalency between the index of refraction (in the visible) and thedielectric constant (in the microwave regime). An electromagnetic wavepropagating in free space has a characteristic wavelength λ₀. When thiswavelength enters a dielectric material with high permittivity and lowloss, the amplitude of the wave is maintained, but the wavelength isreduced λ_(d). In other words, there is little if any energy-transfer,but the wave shrinks between free space and the dielectric (λ_(d)<λ₀).

FIG. 44 is schematic of Φ-wave propagation in different media. In themicrowave regime, one considers the dielectric constant. Metallic filmsof sufficiently small thickness do not reflect microwaves but ratherabsorb or transmit the energy. Similarly to light, metals have aninfinitely high dielectric constant, and therefore the wavelength of anincident microwave frequency shrinks a great amount prior to beingreflected, absorbed or transmitted. However, when a metallic film (of aprescribed thickness) is coated on top of an appropriate dielectric (ofa suitable dielectric constant and low loss factor) a plasmonic effectcan take place.

When a quartz sphere is metallically coated, the plasmonic effect(discussed above) results in a shorter wavelength out put from a sphere.When the metal is coated on top of the same dielectric but in a planarconfiguration, then the same phenomenon occurs and planar plasmons aregenerated.

The thickness of the metal and the dielectric material influence theoutput wavelength. For these reasons, engineered layered structures ofthin metals on top of quartz or intrinsic silicon can create significantdielectric lensing and shrink the incident wave significantly. However,the passage across layers is accompanied by some energy loss.

Dielectric lensing can create focusing and help stimulate up conversionby directing the microwave energy to a selected region of the targetobject. Though the frequency increases, the amplitude decreases, and ifone can afford some energy loss during this conversion, then anupconversion method utilizing dielectric lensing to deliver themicrowave energy in a focused region is suitable for various embodimentsof the invention.

FIG. 45 is schematic of a multi-layer dielectric lens. FIG. 46 isschematic of a Φ-wave propagating through a multi-layer dielectric lens.This schematic representation shows that the incident wave is reduced inwavelength for every paired metallic and dielectric layer (but scatteredin multiple waves). Thus, a dielectric lensing structure in oneembodiment of the invention can be constructed as a multilayeredstructure utilizing processes similar to that in semiconductorphotolithography and development, CVD, ALD and metallization, describedabove. The dielectric lensing can be used to focus RF and MW energy andshorten the incident wavelengths which would help the couplingefficiency to certain organs in the body.

Organic Molecules for Bioluminescence: In bioluminescence orchemiluminescence, the energy for driving the emitted luminescent lightis supplied by a chemical reaction rather than from a source of light.The basic reaction follows the sequence illustrated below with referenceto FIGS. 47-48 . FIG. 47 is schematic of luciferin and luciferase:

-   -   The luciferase catalyzes the oxidation of luciferin;    -   Resulting in light and an inactive “oxyluciferin”;    -   To produce more luciferin, energy must be provided to the        system, here shown as “ATP.”

Sometimes, the luciferin and luciferase (as well as a co-factor such asoxygen) are bound together in a single unit called a “photoprotein.”This molecule can be triggered to produce light when calcium is added toit. FIG. 48 is a schematic of an encapsulated structure 200 of theinvention for bioluminescence. As before, an interface material 202separates compartments 204 and 206. Bioluminescent coatings 208, 210 canbe applied to the encapsulated structure 200. The coatings can obtainoxygen and calcium from nano-particles. In these cases calcium richglass composition or glass composition with surface treatment to addcalcium would be desirable. Techniques for stimulating or entering thetriggering process by microwave “activation” as above can be used.

Microwave Generation and Applicators for Delivery of Microwave Radiationand/or Magnetic Flux to Target Media

In general, microwave appliances have three major components: amicrowave generator, a waveguide and an applicator. Microwaves can begenerated by several methods. Microwave signal transmission can beperformed using transmission lines or waveguides. There are many typesof microwave applicators, each usually designed for a specific use.

Reliable microwave sources (generators) are available nowadays includingmagnetrons, klystrons, Gyrotrons, traveling wave tubes (TWT), backwardwave oscillators (BWO), Cross-Field Amplifiers (CFA), Solid State HighPower Amplifiers and masers. Magnetrons are widely used due to theirproliferation as domestic appliance.

Magnetrons: The magnetron is a diode in which the magnetic field isperpendicular to the electric field existing between the cathode andanode. The magnetic field is created by either permanent magnets or byelectromagnets. The electrons are emitted from the heated cathode andtravel toward the anode at a velocity proportional to the existingdifference in potential. The anode is generally at ground potentialwhile the cathode is at a high negative potential.

Due to the applied magnetic field, the electrons do not travel instraight paths. The charged species traveling at a given velocitythrough the lines of a magnetic field are subjected to a right angleforce called Lorentz's force. The intensity of this force is directlyproportional to the velocity of the charged species and the intensity ofthe existing magnetic field. Its direction is perpendicular to the planeformed by the magnetic and the electric fields causing displacement ofthe charged species. If the magnetic field applied in the magnetron isintense enough (the cut-off value of the magnetic field) the electronscompletely miss the anode and no current circulates in the magnetron.

If the magnetic field strength is adjusted to the cut-off value, and theelectrons fail to reach the anode, the magnetron can produceoscillations by virtue of the currents induced electrostatically by themoving electrons. The frequency of the oscillations is related to thetime it takes the electrons to complete their travel from the cathodetoward the plate and back again. The electrons rotating at a constantvelocity give up energy in the microwave frequency and radio frequencyrange. The microwave energy is coupled by means of a probe from one ofthe resonant cavities into an output coupling antenna where it islaunched into a waveguide.

There are two types of magnetrons; conventional and coaxial. In turn,the conventional magnetrons can be subdivided into three types(cyclotron-frequency, negative resistance and multi-cavity) based on howenergy is transferred to the RF field.

For the cyclotron-frequency magnetron, the diode includes a cathodecylinder inside an anode cylinder. It is positioned between the poles ofa magnet such that the magnetic lines are perpendicular to the electricfield established between the anode and the cathode. Thecyclotron-frequency magnetron operates by virtue of resonance betweenthe period of RF oscillation and the rotational motion of the electron.

The negative-resistance magnetron is also referred to as the split-anodemagnetron, because the anode is split in half. The split plane isparallel to the axis of the anode. This type of magnetron operates onthe principle of the static negative resistance characteristic betweenthe anode sections. It is capable of great output and operates at highfrequencies

The multi-cavity magnetron consists of a cylindrical anode structurecontaining a number of equally spaced cavity resonators. An electrontraveling between the cathode and the anode of such a tube is subjectedto accelerating and decelerating forces resulting in a spiral motionaround the anode, with the electron influenced by all the cavities. Thismagnetron's function depends on the mean velocity of the electron beingsynchronized with the velocity of the traveling-wave component of the RFinteraction field between the cathode and anode. The multi-cavitymagnetron is the microwave tube most commonly used in the microwaveovens and microwave processing systems.

The coaxial magnetron is actually an extension of the conventionalmagnetron structure (cathode surrounded by an anode) with the additionof a third element, a coaxial cavity that surrounds the anode formingthe inner walls. The coaxial magnetron has improved performance overconventional magnetrons. The advantages include: operating mode control,lower fields, decreased arcing, very high quality factor, Q, and ease oftuning. The disadvantages of this tube are its size and weight.

Klystrons: A klystron is a tube based on the velocity modulation of anelectron beam. Klystrons can generate, receive, and amplify radio and/ormicrowave signals. The two basic types of klystrons are the multi-cavityand reflex.

The klystron, in the microwave range, performs the same functions thatordinary vacuum tubes do at the RF range. It takes advantage of thetransit time of the electrons. Electrons are emitted by the cathode andare drawn toward a plate by virtue of a difference in potential. Theelectrons are focused by either magnetic or electrostatic means. Aseries of resonant cavities are aligned next to each other and arebonded by grids and separated from each others by drift tubes. Theelectrons are drawn to the first resonant cavity in which an RF or MWsignal is injected. The electrons couple to the signal and areaccelerated in a one half-cycle and are retarded in the other, thusspeed modulation is achieved. Bunches of accelerated and deceleratedelectrons are formed in the first drift tube. The second resonant cavitybecomes the host of an RF or MW signal and an electric field isestablished in the entrance of the second draft tube, which results in asecond modulation of the beam. The RF or MW energy is extracted at thelast cavity.

Traveling wave tubes (TWTs): A traveling wave tube performs the samefunctions as its predecessors, however, it has an extremely widebandwidth. This broadband amplifier is capable of sweeping a range offrequencies of up to an octave in bandwidth. A bandwidth of one octaveis one in which the upper frequency is twice the lower frequency.

The TWT includes for its major parts: the electron gun assembly, the RFinteraction circuit, the focusing magnets, and the collector. When thecathode is heated it emits a continuous stream of electrons which aredrawn to the anode, and focused into a narrow beam by a magnetic field.

At the same time, the electrons are fed into a tightly wound helix. AnRF signal is injected inside the system. The speed with which the RFenergy progresses along the length of the tube is determined primarilyby the pitch of the helix. The velocity of the RF energy is madesynchronous with the velocity of the electrons, resulting in aninteraction between the electron beam and the RF signal. Some of theelectrons are accelerated under the influence of the alternatingelectric field, others are slowed. As these velocity-modulated electronsprogress through the helix they form bunches, resulting in theamplification of the RF (MW) signal. Some materials processing systemsthat use high power traveling wave tubes (up to 2.25KW) are now widelyavailable. Of all microwave tubes, only the traveling wave tube (TWT)offers a broad bandwidth operation.

Backward wave oscillators and cross field amplifiers: The last two waysof generating MW energy are by backward wave oscillators (BWO) and crossfield amplifiers (CFA). The BWO is used as a local oscillator for theinternal mixing circuitry of spectrum analyzers. The BWO are beingreplaced in many applications by solid state sources. The CFAs aresmall, light, and operate at low voltage. The CFA is capable ofgenerating high peak powers.

MASER (Microwave Amplification by Stimulated Emission of Radiation):When MASERs were invented (1950s), they offered a completely new andrevolutionary method for producing microwaves. The principle ofoperation of the MASER is based on the use of stimulated emission ofelectromagnetic radiation in a medium of molecules or atoms with moreparticles in the upper (excited) state than in the lower state (that is,with an inverted population).

When the particles of the system interact with radiation of frequencyequal to the difference between their ground and excited energy state,the particles are forced to the upper state due to radiation (energy)absorption. When the particles already in the upper state interact withthe radiation, they fall to the lower energy state by emitting radiationof the same frequency as the incident radiation (stimulated emission).

However, in the case of an inverted population, a net excess of emittedradiation takes place over the absorbed radiation, and an amplificationprocess occurs. The radiation emitted in this manner is monochromatic(because of the well defined particles transitions) and coherent(because it is forced by the driving field). The effective couplingbetween the particles and the radiation is achieved by the use of asuitable resonant microwave cavity.

Molecular roto-vibrational states (such as those of excited ammonia gasmolecules) or paramagnetic levels in solid materials (such as the Zeemanlevels of paramagnetic ions) provide the means by which populationinversion is achieved for MASER applications. The frequency of the MASERis therefore dependent on the nature of the molecule (the number ofexcited energy levels and the distance between them).

Gyrotrons & Solid State Amplifiers: Gyrotrons & Solid State Amplifiersare also well known microwave sources that can be used in the invention.

Waveguides: A transmission line can be defined as a device thattransfers energy from one point to another with a minimum loss. Inessence, all transmission lines are waveguides since they are designedto guide the energy wave along a certain direction.

The open two-wire line, the coaxial line, the rectangular waveguide andthe circular waveguide are all used in industry to satisfy specificneeds. The two-wire transmission line consists of two parallelconductors insulated from each other. An open two wire line has threetypes of losses: a) radiation losses, b) dielectric losses and c) copperlosses.

At low frequencies, and over short transmission distances, the open twowire line finds a world wide application, namely the television (TV)twin-lead used to connect an antenna to a TV receiver. The coaxial lineis composed of two concentric conductors separated by an insulatingmaterial.

Coaxial lines are either rigid or flexible. The dielectric in the rigidcoaxial line is usually air. The dielectric in flexible coaxial lines isusually polyethylene. The coaxial lines allow low-loss transmission.There are small dielectric losses in the low frequency coaxial lines,but there are significant dielectric and copper losses as frequencyincreases. But, the coaxial lines offer a compact form factor and can beused for insertion into biological organs.

Waveguides are shielded, capable of low-loss microwave transmission andoffer several advantages over the two wire lines or the coaxial lines. Awaveguide requires no center conductor and its dielectric is usuallyair. Waveguides are hollow metallic tubes and are available in differentgeometric configurations. Waveguide configuration include rectangular,circular and elliptical.

Electromagnetic energy does not move straight down the rectangularwaveguide as an electromagnetic wave; instead, the electromagneticenergy progresses down the guide by a series of reflections off theinternal surface of the narrow dimension.

There are two basic modes of transmission inside rectangularwaveguides: 1) the transverse electric (TE) mode and 2) the transversemagnetic (TM) mode. The TE mode of propagation corresponds to the modein which the electric field is transverse to the direction ofpropagation (the z axis). The electric field lines along the waveguideare parallel to the plane containing the x and y axis. In other words,in the TE modes (also called the H-modes) the Ez=0. In the TM mode (alsocalled the E-mode), the magnetic field is transverse to the direction ofpropagation. The magnetic field loops along the length of the waveguideare always parallel to the plane formed by the x and y axis (Bz=0).

Microwave Applicators: The applicator is a device through which theelectromagnetic energy is transmitted to the target. Its design must beoptimized to ensure high efficiency conversion of MW energy to thetarget.

Aluminum, copper and stainless steels are widely used in the fabricationof commercially available applicators. The irradiation of the targetarea has to be engineered carefully to excite and sustain the electricfield patterns of interest. The applicator is very dependent on theapplication and how the desired irradiation is defined.

Multimode applicators find world-wide applications covering almost everyapplication of microwave power. Single mode applicators or resonantcavities are designed to sustained well defined field patterns. Theestablishment of a well defined electric field pattern inside themetallic enclosure in single mode cavities allows uniform heating ofsamples having small dimensions.

The quality factor of an applicator, Q, of a resonant circuit at thefrequency of resonance is defined as:

Q=2π (energy stored/energy dissipated per cycle).

Magnetic Flux Applicators:

One simple magnetic flux applicator of the invention is a multi-turnsolenoidal coil. FIG. 49A is a schematic of a multi-turn solenoidal coil220 showing the projection of the magnetic field along the longitudinalaxis. FIG. 49B is a schematic of another multi-turn solenoidal coil 220showing the projection of the magnetic field along the longitudinalaxis. A target to be treated would be placed along the longitudinalaxis. FIG. 50 is a schematic of bird cage coil 230 showing theprojection of the magnetic field in a radial direction. A target to betreated would be placed along the radial direction. There are various RFcoils used for magnetic resonance which can have application to theinvention for delivery of magnetic flux to the target. Each coilconfiguration has advantages and disadvantaged depending on theapplication. These coils include but are not limited to: Alderman-GrantCoil, Bird Cage, Butterfly Coil, Dome Resonator, Gradiometer,Implantable, Inside Out (Schlumberger Coil), Intravascular Coil, Ladder,Loop-Gap Resonator, Loop-Stick, Meanderline, Transmission Line (TEM)(Slotted Tube), Truncated Spiral, Superconducting Coil, Mouse Coil,Multi-Turn Solenoid, Ribbonator, Phased Array Volume, Saddle Coil,Scroll Coil, Single Turn Solenoid, Surface Coil and Spiral Coil.

The bird cage coil construction has been routinely used in practice forMRI imaging of the head and brain. Meanwhile, the single turn solenoid,which is a single-turn solenoid (STS) is a tubular inductor with acapacitive gap running along the length of the tube, has been used forextremity exposure, such as the breasts and the wrist. The phased arraycoil allows the coupling of energy with more controlled method forcoupling to various species within a media.

MRI machines are particularly attractive as noted above, given theindustrial base in existence in the medical field. A conventional MRIdoes not use of ionizing radiation to produce images. However, aconventional MRI does make use of strong magnetic fields, radiofrequency energy, time varying magnetic fields, magnetic fieldgradients, cryogenic liquids to cool the magnets (to produce very strongmagnetic fields).

The installed base of MRI equipment is estimated at more than 10,000units. The number of MRI scans exceeds 75,000,000 MRI scans per yearworldwide. Original Equipment Manufacturers (OEMs) of MRIs include amongothers large multinational companies including: General Electric MedicalSystems, Siemens Medical Solutions, Toshiba Medical Systems, PhilipsMedical Systems, Hitachi Medical Systems and Fonar.

When gases are ionized (or formed into a plasma) and electrons are freedfrom the binding energies of their respective nuclei, the electrons cantravel with a mean free path that depends on the pressure within thecontainment chamber and the nature of gas. Furthermore, electron in thepresence of a magnetic field (as applied from an MRI machine) can entera precession motion or ECR, as discussed earlier. The ECR frequencydepends on their masses and is dependent directly on the magnitude ofthe magnetic field.

FIG. 51A is a schematic of a MRI arrangement suitable for the inventionand representative of a typical commercial MRI system. In one embodimentof the invention, a target medium or a patient 300 is placed on aprecision table 302 (that has for example an accuracy of 1 mm). Thetable 302, with the target or patient, is introduced in a largecylindrical structure containing a magnet 304 with a very homogeneousmagnet field in the axis of the magnetic cylinder. Superconducting coilsare typically used in the MRI machines to produce the strong magneticfield from 1 Tesla to 11 Tesla. In one embodiment of the invention, theapplied magnetic field from the MRI is applied in conjunction with amicrowave field or a radio frequency field to induce a plasma in the upconversion gas containers of the invention. FIG. 51B is a schematic ofproviding more operational detail to the MRI arrangement shown in FIG.51A.

The operation can be computer controlled by computer 306. The RFcomponents including the radio frequency source 308 and pulse programmer310 can be adjusted. The RF amplifiers 312 can increase the pulses powerfrom the mW range to the kW range, which is typical of RF powers in MRIimaging, where the presence of a Radio Frequency pulse (in the MHzrange) with an orientation 90 degrees and 180 degrees orientationvis-à-vis the uniform and axial magnetic field can be used to generateplasmas in the gas containing UCC structures of the invention. As withthe commercial MRI imaging, the magnetic fields (or gradients thereof)in one embodiment of the invention would be computer controlled in termsof the shape and amplitude of each of the three gradient fields.

In one embodiment of the invention, it is advantageous to include gaseswith characteristics such as: para-magnetism, unpaired electrons,asymmetrical charge distribution, well pronounced electrical dipoles,low ionization potentials and the ability to emit in the UV range. Inone embodiment of the invention, gas isotopes can be contained in thegas containers. For example, Xe¹²⁹ has been demonstrated to be quitesuccessful as an imaging gas for MRI. Thus, in this embodiment,conventional MRI can be used to image the position of the UCC structuresin the target organ before microwave or RF activation.

It is possible to use MRI techniques with materials other than Xe¹²⁹ toensure that the delivery of bio-therapeutic agents has been successfullyaccomplished. For example, it is possible in one embodiment of theinvention to use magnetic materials or ionic species with magneticproperties, as part of the silicate structure of the UCC materialcomposition to act as tracers for imaging. When using magnetic “dopants”for imaging in MRI, care is taken to ensure that magnetic tracers havethe right concentration in order to avoid causing magnetic inductioneffects that may in turn lead to heating. The concentration of Fe³⁺ inthe ppm level compared to the silicate network formers ought to besufficient for imaging but not for localized over heating and magneticinduction.

After the imaging step using MRI is performed, the activation processusing microwave and RF can be executed to achieve up conversion;however, the UCC can contain an up converting media (such as gases proneto ionization leading to plasma generation and hence UV emission) and adown converting media (such as doped Y₂O₃) at the same time. FIG. 52shows a UCC structure 400 including a capsule-type region 402 forholding an upconverting gas (not shown) and a down converting media 404.In this embodiment, an X-Ray treatment can be used to induce a desirabledown conversion to generate UV emissions in the proper range suitablefor photo-activating chemotherapeutic agents of choice 410, as shown inFIG. 53 . More generally, FIG. 53 is a schematic of a UCC structureincluding a capsule-type region for holding an upconverting gas and adown converting media where an activatable agent is attached thereto.

Magnetic Field Induction:

FIGS. 54-1A to 54-11 are a group of schematics depicting variousprocesses for depositing a magnetic membrane structure according to oneembodiment of the invention. The process is similar and uses many of thetechniques discussed above with regard to FIGS. 13-22 .

In FIG. 54-1A, a carrier wafer 30′ having a release layer 32′ andstarting wafer 34 disposed thereon is provided. A mask 35′ is depositedand thereafter has an opening defined thereon to expose the startingwafer 34′. A wet etch is used to generate the undercut portions 36′. InFIG. 54B, a plasma etch is used to generate the undercut portions 38′.Differences between wet etch and plasma etch have been discussed before.Plasma etching is anisotropic and leads to a trench definition havingmore rectangular edges than typically possible with wet etching. A mask34′ is deposited and thereafter has an opening defined thereon to exposethe starting wafer 32′. As shown in FIG. 54-1A, a dry etch is typicallyused to generate the trench-like portions 36′.

In FIG. 54-2A, deposition of a magnetic film 500 occurs using forexample molecular beam epitaxy (MBE) or by alternating target laserablation deposition (ATLAD) c to deposit for example a BaFe_(10.5)Mn_(1.5)O₁₉ film. The BaFe_(10.5) Mn_(1.5)O₁₉ film has a suitably highmagnetic susceptibility and would therefore couple efficiently toelectromagnetic frequencies described below. Other magnetic materials(as discussed below) can also be used in various embodiments of theinvention. Alternating target laser ablation deposition is describedelsewhere and the following patent documents describing alternatingtarget laser ablation deposition are incorporated herein by reference intheir entirety: U.S. Pat. No. 5,173,441 and U.S. Pat. Appl. Publ. No.2004/0033702.

Other magnetic films and magnetic materials are also possible in variousembodiments of the invention. Examples of such materials include but arenot limited to: Fe—Si—Al materials (in a flake or other form),ZnCo-substituted W-type hexaferrite materials, Fe₂O₃ materials(including particles and nano-particles of oleic acid hydrophobizedmagnetic Fe₂O₃), cobalt ferrite materials (including particles andnano-particles of cobalt ferrite CoFe₂O₄), Fe/Cr materials includingmultilayered films of Fe/Cr, Fe—Ag materials including Fe—Ag films,Fe—Ag materials having giant magneto-resistance (GMR effects),FexAg_(1-x) alloys (x-0-0.045) materials (for example fabricated usingan electron beam co-evaporation technique), a ferrite series of[Ca(CoTi)_(x)Fe_(12-2x)O₁₉]_(96.0)[La₂O₃]_(4.0) ferrite with x carryingfrom 0 to 1.0, and materials (including particles and nano particles) ofFe³⁺ for example produced by a fermentation process such as described inU.S. Pat. No. 6,444,453, the entire contents of which are incorporatedherein by reference.

Electron beam co evaporation techniques are described in U.S. Pat. Appl.Publ. No. 2002/0110698 and U.S. Pat. No. 7,393,416. The entire contentsof which are both incorporated herein by reference.

The magnetically coated wafers described in FIG. 54-2A and FIG. 54-2Bare then etched to remove the mask layer through the use of solventleading to lift off of the mask layer 35′. A magnetic film 500 isdeposited within trench 36′, and trench 38′ is left behind. The wafer issubsequently cleaned and caped using wafer 40′ using methods similar tothose described before in FIG. 15 .

FIG. 54-3A and FIG. 54-3B are schematics showing how after removal ofthe patterning resist, the starting wafer can be capped with the plate40′ (e.g., a flat quartz wafer) to form gas containers. The wafers inFIGS. 54-3A and 54-3B are removed flipped and transferred to anothercarrier wafer 31′. This is accomplished by removing the wafers 30′ fromthe release layers shown in FIGS. 54-3A and 54-3B, after having beensubsequently transferred to another carrier wafer 31′ with anotherreleased layer 33′ as shown in FIGS. 54-4A and 54-4B.

FIG. 54-5A is a schematic showing another embodiment of the inventionand depicting after removal of the resist, that two mirror imaged wafers42′, 44′ (using a wet etch) are joined to form the gas containers withthe resultant magnetic membrane 500 in the middle. A more roundedcontainer can be obtained prior to removing the release layer. FIG.54-4B is another schematic showing that, after removal of resist, twomirror imaged wafers 46′, 48′ (using a dry etch) can be joined to format least one gas container.

FIG. 54-6 -A is a process schematic showing the release layer 32′ havingbeen removed, followed by patterning at step 54-6-A, the masking, andpatterning at step 54-6-B, and the etching at step 62-6-C to release andseparate the UCC structures from each other. In this embodiment, a dryetch is used to obtain the gas containers.

FIG. 54-7 is a process schematic showing two gas containers 50′, 52′ ofthe invention made using the large scale repeatable and reproducibleprocesses discussed above. The gas containers 50′ and 52′ containmagnetic membranes 500 separating the two cambers within a gascontainer.

FIG. 54-8 is a process schematic showing the filling of the gascontainers 56′, 60′ with the appropriate gases prior to sealing. In FIG.54-8 , each of the as containers 56′, 60′ have magnetic films containedwithin the sealed structure. FIG. 54-9 shows the treatment of thegaseous-filled up converters (for example with an HF treatment) to roundthe edges.

FIG. 54-10 describes the process through which a magnetic film 500″ isdeposited on the inner walls of the UCC. In this example, thefabrication process uses two mirror image coated wafers 34″ with amagnetic film as depicted in FIG. 54-10 -B. In this example, acontinuous coating is provided around the inner walls of the UCC. ThisUCC structure 56″ in FIG. 54-10 -C can be treated with HF to yield a UCCwith more rounded outer wall 62″ as illustrated in FIG. 54-10 -D.

The construction steps of a UCC with a single magnetic membrane areprovided in FIG. 54-11A to FIG. 54-11 -G. In this example, the wet etchprocess performed on wafer 34′″ is continued until the etching frontreaches the outer wall of wafer 34′″. Subsequently a magnetic filmdeposition is performed (similar to the deposition techniques describedin the previous figures) to layout a magnetic membrane. The wafer 34′″having a magnetic membrane is sealed in the presence of a preselectedgas. The sealing process typically involves pressing wafer 34″ againstwafer 40′″. The formed composite shown in FIG. 54-11 -C is then releasedfrom release layer 32′″ and then sealed against a mirror wafer 34′″ thatdoes not a magnetic coating (see FIG. 54-11 -D). The sealed wafers aredetached from release layer 32′″. The wafers shown in FIG. 54-11 -E areetched to yield UCC structures 52′″ in FIG. 54-11 -F. The UCC structures52′″ can be HF treated to yield the resultant UCC structures 62′″ inFIG. 54-11 -G.

Similar to the previous descriptions, the UCC 52″, 52′″, 62″ and 62′″are compatible with Au coating techniques described before for singleand double Au shells that can lead to plasmonic activity. FurthermoreUCC 52″, 52′″, 62″ and 62′″ can have CNT attached to them using similartechniques to those described before.

The magnetic films depicted in the embodiments shown in the FIG. 54group of schematics (described above) form a double or a single membranewithin the double gas container structure. In other embodiments of theinvention, a UCC structure only needs one magnetic layer and one gascontainer. In either case, upon heating, the magnetic membranes would bestressed above their modulus of rupture to break the barrier between thetow chambers within the UCC. Once this barrier is broken the chemical(s)that were separated now chemically react. For example chemiluminescentmaterials are made to react and emit light upon breaking the magneticbarrier.

In other cases, the magnetic barrier of strong susceptibility (orabsorption) can assist in plasma ignition of gases. For the case of thedouble gas container structure, the rupture would lead to the merging ofthe two chambers formed within the gas containers. Upon rupture, themagnetic membrane would release for example magnetic flakes and/ormagnetic particles. These magnetic flakes and/or particles are expectedto participate in further magnetically induced rotation or RF/MW andmagnetic induction thorough dipolar coupling of energy. Either onemechanism would lead to further heating causing more friction with theappropriate gas chemistries and ultimately leading to plasma ignition.

Similar to what was described before the gases such as Ne, Xe, He, Hg,H₂, N₂, Ar, Kr can be used as the fill gases. Also gas mixtures Ne+He,Ne+He+5% Xe, Ne+5-10% Xe can be used. The percent Xe addition is byatomic percent. Hg+Ar emit at the 360 nm; Ne+1% Ar also emits at 365 nm.Furthermore, other gas combinations can be used, including iodine vaporwith various impurities. After the gas fill, the gas containers can betreated to an HF solution to treat their edges to produce the UCCstructures 62′, 64′.

FIG. 55 is a side view schematic showing that the shape of up converterstructures of one embodiment of the invention having magnetic layers 500contained therein can be controlled and further illustrating thatelongated and spherical shapes can be manufactured in a reproduciblemanner. FIG. 56 is a side view schematic showing that the magneticallyloaded containers can be coated with Au for single coating or a doublecoating 502, both of which can lead to plasmonic resonance effects.Similar to the descriptions and examples provided before, the outersurfaces of the gas containers (which in this embodiment can includemembranes or particles with magnetic properties) can be coated withmetallic coatings of Au and Ag for plasmonic activity. It possibletherefore in this embodiment, through similar or identical process asdescribed before, to also achieve a single metallic or a double metalliccoating for plasmonic resonance.

Similar to the descriptions and processes described before, the upconverter structures (in this embodiment where the up converters includemembranes or particles with magnetic properties) can be built to includecarbon-nano-tubes (CNTs) which can protrude inside the enclosure. TheseCNTs are added for the purpose of facilitating the RF/MW coupling andplasma ignition or initiation. FIG. 57 a top view schematic showing ofthe shape of up converters having magnetic layers 500 contained therein.The shapes can be controlled. In various embodiments, elongated shapesand spherical shaped up converter structures can be manufactured in areproducible manner using the lithographic techniques described above.The attachment of CNTs is illustrated for both shapes shown in FIG. 57 .

The magnetic films 500 respond to an oscillating magnetic field forexample in an electromagnetic wave of an alternating magnetic fieldgenerated using the flow of alternating current flow inside a solenoid.The energy coupling of a magnetic material to the electromagnetic waveof an alternating B field is characterized by the magneticsusceptibility of the film. A couple of factors affecting energycoupling are magnetic permeability and magnetic loss. Almost allmagnetically susceptible materials readily absorb RF/MW because RF/MWradiation are electromagnetic waves that have an electric field and anorthogonal magnetic field of the same frequency.

Typically RF applicators operate at low frequencies below 110 MHz andoperate up to 300 MHz, at which point in frequency the energy cantypically no longer be contained between ground and the electrically hotelectrodes. While the demarcation between RF and MW is not exact interms of a definition, it is generally agreed that at 100's of MHz, theelectromagnetic radiation is characterized as MW electromagneticradiation. MW radiation typically propagates from and is not confined bythe generating network. Frequencies in the microwave regime propagate infree space unless the MW radiation is contained inside an enclosure.

There are various ways of building the RF applicators of the invention.The configuration of the RF electrodes can easily be modified and cantake different size and shapes. In general, the length of the electrodedoes not impact the uniformity of the RF field distribution. Over alength of one meter, the voltage across an electrode would drop by lessthan 3% which is negligible. The RF generators can also vary; butbecause of the stability of solid state generators and their wide useenabled through wireless applications and cell phones, solid stategenerators are cost effective and often utilized to power electrodes inan RF applicator. Some RF applicator configurations of interest aredescribed below.

FIG. 58 is schematic of an RF plate capacitor configuration. Parallelplate electrodes 602 can be any dimension and can be used to apply froman RF source 604 an electric field of small to high strength. FIG. 59 isa schematic of an RF stray field applicator configuration. The electricfield is strongest between the electrodes 606, 608 and decay in strengthwith distance from ground to the powered electrode 608. Alternatively,FIG. 60 is a schematic description of a staggered RF stray fieldapplicator configuration. The electric field is redistributed in threedimensions, and is no longer predominantly confined to a plane.

The capacitive plate, the stray field, and the staggered stray fieldconfigurations could be used to treat (for example) tumors that areclose to the surface and that are not deep within the body. Other RFapplicators capable of deep treatment (as discussed below) may be moredesirable for controlled treatment and plasma initiation of the gaseousmedia if the tumor site is deep within the body. The RF applicatorscapable of deep treatment may also be capable of treating the surface.

FIG. 61 is a schematic description of a hybrid RF applicator whereadjustable electrodes are illustrated. This configuration allows moreflexibility as compared to the RF configurations shown above. The heightbetween the electrode 608 and ground electrode 610 can be adjustable.Alternatively, FIG. 62 is a schematic description of a staggeredcylindrical RF applicator configuration. The electrodes 606, 608 arepositioned in a circular/cylindrical pattern which provides more controlover the deliverable energy patterns.

FIG. 63 is a schematic description of a cylindrically configuredstaggered cylindrical RF applicator. The electrodes 606, 608 arepositioned in a circular/cylindrical pattern which provides more controlover the deliverable energy patterns. The size of this applicator can bevariable depending on the size of the part of the workpiece or humanbody to be treated or if the workpiece or entire human body is to betreated.

FIG. 64 is a schematic description of a cylindrically configuredstaggered cylindrical RF applicator configuration. The electrodes 606,608 are positioned in a circular/cylindrical pattern which provides morecontrol over the deliverable energy patterns. Three sections 620, 622,and 624 power the electrodes 606, 608. The size of this applicator canbe made variable depending on the size of the part of the workpiece orhuman body to be treated or if the workpiece or entire human body is tobe treated. Furthermore the control of the applicator is accomplished insections such that the RF treatment can be performed in series, witheach controlled section powered sequentially and programmed to deliver asuitable recipe in terms of power and frequency.

The RF applicator with sections 620, 622, and 624 operating in phase canbe operated over a large frequency range and depending on the site to betreated and the magnitude of the operating magnetic field. Differentfrequencies may be used !! the higher the magnitude of the magneticfield, typically the higher frequency the operational frequency whichwould be used.

The three sections 620, 622, and 624 can also be powered out phase. FIG.65 is a schematic of a phased RF applicator capable of deliveringdifferent frequencies. The waveform used in the generators depicted inFIG. 65 can be controlled at a centralized computer controller to injectprogrammable phase delays between the various electrodes.

In FIG. 65 , the electrodes can be made to operate independently or insynchronization with one another. The electrode sets corresponding toone generator can be made to operate in phase or out of phase. Thegenerators themselves can be pulsed on and off as may desirable by atreatment recipe. A switching network can be utilized to energize theelectrode by one set of frequencies for a period of time and then switchto another set of generators to operate at a different frequency regime.The first regime could be in the KHz, and the second regime could be inthe MHz.

In one embodiment of the invention, the RF applicators can be adjustablein frequency provided that the generator is capable of doing so. If not,separate generators (capable of delivering power at differentfrequencies) can be utilized to energize the electrodes.

The RF applicators shown above are capable of delivering a large amountof powers in a short pulse as needed. The microwave applicators and theRF applicators can be designed to work in conjunction with an MRImachine (such as the one described above) to take advantage of thecapability of the magnetic gradients and the uniform cylindricalmagnetic field.

In one embodiment of the invention, the RF and MW applicators areconfigured with a preferential orientation of the electric field, wherethe electric field is orthogonal to a cylindrical magnetic field. Inthis configuration, the electrons generated during plasma generationprecess along the magnetic field lines.

Targeted Magnetic Field Applications

It is possible to exercise various aspects of the invention without theneed for an MRI machine. In these embodiments, the utilized magneticcoils can constructively trigger rotational movements in the gasescontained in the UCC structures. Various ways of triggering a magneticfield can be applied constructively to achieve the desired result. Byconsidering a coil magnet first, a series of coils magnets can beenergized using current flow. In this case, no MRI machine is needed togenerate the up conversion.

In various embodiments, multi-head coils are operated at low frequencyfrom 1 KHz to 400 MHz and are engineered to be out of phase with oneanother. Furthermore, the magnetic fields emanating from each coil canhave different (or similar) orientations. The resulting magnetic fieldorientation hence formed in this series of magnetic coils (that areoperable out of phase with one another) can lead to the triggering ofmagnetic field pulses each in a different orientation. In oneembodiment, each magnetic field pulse tends to orient the paramagneticgases, the magnetic dipoles within the magnetic films, and/or magneticdipoles of the magnetically susceptible nano particles. The series ofthe magnetic coils is designed to orient the magnetic dipoles (containedwith the UCC structures) in a synchronized fashion for maximizedcoupling and the inducement of rotary movement of gases which can leadto collisions and plasma ignition.

The number of magnetic heads can be made variable depending on thesusceptibility of the UCC. The more susceptibility the less number ofmagnetic head needed to trigger plasma ignition and up conversion. Themagnetic heads can be made close or far apart depending on theapplication (treatment).

FIGS. 66A, 66B and 66C are schematics of different sets of solenoidcoils in different configurations designed to excite and stimulaterotational movements of paramagnetic gases and the magnetic dipolescontained in magnetic films and magnetic nano particles that are in turnformed as part of the UCC structures of the invention, described above.

In FIG. 66A, three solenoids 702, 704, 706 are configured in a circleand oriented such that their respective protruding magnetic field isoriented toward the general direction of the center of the circumferenceformed by the three coil magnets. The magnetic field can protrudeslightly off center. In FIG. 66B, four solenoids 702, 704, 706, 708 areconfigured in a circle and oriented such that their respectiveprotruding magnetic field is oriented toward the general direction ofthe center of the circumference formed by the four coil magnets. Themagnetic field can protrude slightly off center. In FIG. 66C, fivesolenoids 702, 704, 706, 708, 710 are configured in a circle andoriented such that their respective protruding magnetic field isoriented toward the general direction of the center of the circumferenceformed by the five coil magnets. The magnetic field can protrudeslightly off center.

In one example of this embodiment of the invention, these five solenoidscan be employed in a way that maximizes the torque applied to themagnetic dipole and dielectric dipole. In this case a solenoid #1 (702)would be activated followed by solenoid #3 (706), followed by solenoid#5 (710), followed by solenoid #2 (704), followed solenoid #4 (708)followed by solenoid #1 (702); so fort and so on. In other words, everyother solenoid is sequentially activated. The solenoids to be poweredwould then operated out-of-phase to be able to take full advantage ofthe rotary motion imparted to the magnetically susceptible matter in theUCCs.

FIG. 67 illustrates the operation of a series of coil magnets that isout-of-phase. Indeed, FIG. 67 is schematic of configuration forserialized operation of four coil magnets operating out of phase withone another to maximize the rotational imparted into the magnetic anddielectric matter contained in the UCC. This configuration can be usedfor the purpose of igniting a plasma for a brief interval of timesufficient to photo initiate an agent in the medium of the UCCstructure, and in particular for activation of therapeutic agent, with atime frame not sufficient to cause tissue damage.

The RF, MW or magnetic susceptibility of nano particles or carbon nanotubes that can be engineered within the UCC can assist in heating andlowering the ionization of gas mixtures described elsewhere and canfacilitate plasma ignition. Furthermore, as in the embodiments describedabove, a number of different gasses can be used to generate the neededlight emission to activate therapeutic agent or other activating agentin the medium about the UCC structure.

To further elaborate on the coil magnets and the mechanisms thereofcapable of constructively operating to trigger up conversion by plasmainitiation; other configurations and modifications are described below.

In one embodiment, two coils are made to operate simultaneously incooperation with one another. In this case for the five solenoidsexample, solenoid #1 and solenoid 3 are operated at the same time indifferent direction (this is done by circulating an electrical currentin solenoid #1 and a current in the opposite direction in solenoid 3) insuch way to create a re-entrant magnetic field path as illustrated ofFIG. 68 (see solid magnetic line). In a similar fashion, the magneticfield between 2 and 4 forms a reentrant magnetic field (see brokendashed magnetic line) and in turn the magnetic field between 3 and 5forms a reentrant magnetic field (see broken dotted magnetic line).

The waveform used in the generators depicted in FIG. 68 is controlled atthe centralized computer controller to inject programmable phase delaysbetween the various coils. The current fed into select coils can be inphase with one another, or out of phase with one another or have a phasedelay between a pair of coils. In the example shown in FIG. 68 , thepaired coils 1 and 3 are 180° out of phase and operate simultaneously.In the same example, the paired coils 2 and 4 are 180° out of phase andoperate simultaneously. However, the operation of the two pairs can be90° out of phase. In this manner, the various generators operate in acontrolled manner and have engineered reentrant magnetic field pathways.

FIG. 69 is a schematic of two electromagnetic coils working inconjunction with one another to form a reentrant magnetic field whichcan penetrate an object when the field emanates from one coil to theother. In general, reentrant magnetic fields can be formed from manycoil and magnet configurations. The configuration selected would dependon the number of electromagnetic coils juxtaposed in a constructive way.The higher the number of electromagnets, the more flexibility one has inengineering a magnetic path that is suitable for use through a workpiece, a patient or a part of a work piece or a part of a patient.However, in one embodiment of the invention (as illustrated in FIG. 69), a reentrant magnetic field can be achieved by only twoelectromagnetic coils. This configuration would be suitable for exampleif the patient or one of the patient's part is outside of the coils. Inother words, a reentrant magnetic field would be used when the workpiece or patient or any part of the work piece or patient is to be leftoutside of the coil region for treatment.

If a large number of magnets is used, then in one embodiment of theinvention a large number of configurations (i.e., available magneticpath ways) are possible for directing and collimating the magneticfield. FIGS. 70A and 70B illustrate a configuration with a series ofcoil magnets or electromagnets which can be used to engineer a varietyof magnetic patterns that can be time varying patters according to theway the electromagnets are powered. In particular, FIG. 70A is aschematic depicting a large number of electromagnets (16 electromagnets)that can be disposed around a work piece or a patient to create a largenumber of magnetic path ways. In particular, FIG. 70B is a schematic ofa magnetic configuration illustrated for aligning the magnetic field andfor strengthening the magnetic field for an elapsed amount of time.Conversely, a large number of electromagnets can be used around the workpiece or patient to create other magnetic path ways that are useful.

The magnetic field achieved in FIG. 70B can be used to perform the samefunction as the one described in FIG. 68 (where by certain magneticcoils are operated out of phase to achieve rotational energy coupling togases and to lossy magnetic and dielectric matter). However, another usefor this multipath-way magnetic design is to concentrate the magneticfield sufficiently in one localized area of a work piece or a patient,to thereby reach a sufficiently high magnetic field strengths (e.g., atleast 0.5 Tesla) which would permit the use of an additional gradientelectromagnet in conjunction with RF to trigger a plasma and/or tocreated a plasma with ECR conditions.

FIG. 71 is a schematic depicting the utilization of variable fieldstrength multipath-way magnets and their use in conjunction with eachother. FIG. 72 is an illustration of a configuration where a largemultipath way magnet can be used in conjunction with a (relativelysmall) reentrant electromagnet for the purpose of triggering upconversion. The multipath-magnet (when operated in a focused mode) couldreplace the role of an MRI, and would be more cost effective due to itssimplicity and basic hardware and computer control. The multipath-waymagnet can be used with two reentrant magnets, in this embodiment, toachieve up conversion of a gaseous media in the UCC structure of theinvention. The multipath-way magnet would be congruent with the use offour of five phased reentrant solenoids.

In the case of relatively smaller reentrant magnetic coils, as describedbefore, FIGS. 73A and 74B are schematics of various sets of solenoidcoils each arranged in a configuration to treat local parts of an objectsuch as for example a human patient. The serial magnetic coil approachcan be applied to localized parts of the body in this case smaller coilsconfigured closer to one another can be used to achieve maximumcoupling.

FIG. 73C is a schematic showing four magnetic coils spaced apart to hosta patient and operate in series for the purpose of a targetedpenetration into a work piece or patient and for the triggering of aplasma in the UCC structures of the invention to initiate abio-therapeutic agent. In the above magnetic flux and RF/MW embodiments,it is of concern (when the object treated is a patient instead of anartificial medium) the quantity of the dose of RF and magnetic fieldapplied. FIG. 74 is a schematic of a temperature, electric field, andmagnetic field probe all of which can be measured simultaneously byfeeding the difference in temperature rise between the two adjacentprobes in the illustration to a computer and deriving the local fieldstrength, one probe has a material susceptible to oscillating electricand magnetic fields while the other probe is measuring the environmentaltemperature. In FIG. 74 , magnetic field strength and or the electricfield strength can be measured using two fiber optic probes one withelectromagnetic susceptible tip and the other one with air to act as thereference. The temperature rise and hence the difference between the twoprobes can yield the electric or magnetic field strength; hence, thetreatment dose. If the probe is inserted inside a patient's body, thenthe environment temperature measured by the probe becomes the patient'sbody temperature and the electromagnetic energy is measured by thedifference in the temperature between the two adjacent probes inside thepatient's body.

FIGS. 75A and 75B are schematics of sensors (including temperature,magnetic and electric field strengths) employable in various embodimentsof the invention. The probes shown in these figures can be implanted inthe body and positioned below and above the patient for mapping theenvironment of a patient or another workspace. The probe sensorinformation could be provided to the computer 306 shown in FIG. 39 , forexample, to be part of the treatment monitoring.

FIG. 76 is a schematic of an area array (mesh) of sensors provided underand above the patient to make precise measurements. This area array ofprobes can be use to ensure that the dose and the radiation is deliveredto the patient at the deigned place and per the programmableinstructions. In one embodiment, any deviations from what is deemed theprocedure of record, an emergency shut down can be triggered.

In one embodiment of the invention, multiple probes can be used aroundor inside the patient to monitor the patient temperature andelectromagnetic dose received during the treatment. This information canbe used as feedback to the computer to regulate the Pulse width durationand frequency selection. In one embodiment of the invention, RF and MWare used sequentially, simultaneously and possibly with magneticinduction depending on the composition of the UCC. Once a dose isestablished (a dose calibration is done) the internal probes above andbelow the patient we can calculate the absorption in the patient withouthaving to insert a field measurement probe inside a patient.

Three probes are shown: below, inside. and above the patient to monitorthe patient temperature and feedback information to the computer toregulate the pulse width duration and frequency selection. In oneembodiment of the invention, RF and MW are used sequentially,simultaneously and possibly with magnetic induction depending on thecomposition of the UCC. Once the probes above and below are calibrated,the absorption in the patient can be calculated without having to inserta field measurement probe.

FIG. 77 is a schematic of the utilization of magnetic induction if apatient requires treatment in a limb and not an internal organ. In a fewcases, when the tumor is located the arm or the leg, it is possible touse magnetic induction using one coil. In this case a solenoid isactivated using an alternating current and low frequencies (anywherefrom the kHz to the MHz) to trigger the gaseous up conversion. A nonpolar liquid bag can be used with this local applicator around the siteto be treated. De-ionized water can also be used with this localapplicator.

Macroscopic Probes

While illustrated above with regard to microscopic size plasmacontainments, the invention is not limited to that size gas or plasmacontainments. For many applications, microscopic size plasmacontainments still provide unique advantages. The advantages here relateto the capability of the invention to initiate plasmas under conditionswhereby ordinarily one would have not expected plasma ignition to bepossible. As described above, the magnetic fields in conventional NMR orMRI machines had not been realized prior to the invention as beingcapable of participating in the igniting and sustaining a plasma(especially inside a medium and especially inside the human body). Yet,this work has realized this capability in millimeter and sub-millimetersize plasma containments.

In one illustration, a static magnetic field from a commercial MRI wasused in conjunction with and RF source able to supply from 100 MHz to400 MHz. The microwave power supply was connected to various antennasplaced within the bore of the MRI magnet to ignite and sustain plasmacontained within glass containers. In some cases the gas container wasplaced inside of a phantom and in others the gas container was in thevicinity of a well plate containing a cell culture and a photo-activatedbio-therapeutic agent. RF power was supplied from the antenna. Whiledemonstrated with magnetic fields from a commercial MRI, similar resultsin the presence of magnetic fields from rare-earth permanent magnets(with a magnetic field strength of about 1.5 Tesla) have been realizedat remarkably low powers. In the presence of a magnetic field such asthe MRI plasma were sustained inside glass containers at 5 Watts asopposed to 50 Watts.

While demonstrated with static (non-time varying) magnetic fields fromthe MRI (or permanent magnets), various embodiments of the inventionvary the magnetic field in time, with spatial gradients to producemagnetic induction effects which can assist in the ignition and/ormaintenance of a plasma in the gas container up converters of theinvention. Additionally, motion of the gas container up convertershaving an electrode attached to it or a metallic loop relative to themagnetic field can likewise produce magnetic induction effects which canassist in the ignition and/or maintenance of a plasma in the gascontainer up converters of the invention.

Some work was also conducted in a modified commercial microwave oven tohave feed-through to have a mechanical rod to move magnets around a gascontainer and to have the antenna of a Tesla coil reach inside thechamber and in proximity to the a phantom containing a gas container.The feed-through holes were equipped with chokes to eliminate leakage.The microwave antenna was polarized using an extended waveguide insidethe cavity. In some of these cases, a fluidic conduit was connected to aglass tube that was not sealed and the open ends of the gas tubes wereconnected to a vacuum side on one side and the gas feed on the other. Inthis case scenario a plasma was generated having open ended ends thatwere connected to the appropriate pressure control and gas feed.

In this work, sealed glass tubes made of boro-silicates,soda-lime-silicates, lead glass, and quartz tubes of dimensions rangingfrom 30 mm down to 4 mm in length, and from 3 mm in thickness down to900 microns in thickness. The sealed glass containers were evacuated andbackfilled with a mixture argon, nitrogen, hydrogen, mercury vapor andsodium. The vacuum pressure ranged from 5 mTorr to 10 Torr. These gascontainers were placed inside an MRI from GE Healthcare Technologies dModel 1.5T SIGNA MRi EXCITE HDx. In some cases we showed sustainedplasma after ignition with a Tesla coil outside the bore of the magnetand in some cases they were ignited and sustained inside the bore of themagnet with a Tesla coil.

In one embodiment of the invention, the sealed containers were subjectedto a cleaning process to “burn-off” organic contaminants from the innerwalls of the containers. The cleaning process involved the followingsteps: placing electrodes at the end of the container, sealing theelectrodes into the end of the container through a gas heated flame,followed by cooling and then performing a vacuum drawing followed by thebackfill of the container using the desirable gas and gas mixtures likeargon or nitrogen, and by adding any additives that could lower theionization potential of the gas, then the electrodes on each side thetube were hooked up to a high voltage low current transformer to ignitea plasma and heat the tube using both the plasma and an external heater.The plasma was ignited and sustained with a 400 milliamps, 12,000 volt,350 EC. The temperature of the containers was monitored each time to 400EC on the outside. The internal temperature was exceeding 700 EC atwhich organics are decomposed. The container is then allowed to cool.The containers were then placed on an insulated table and heated locallyby a high temperature flame to temperature sufficient to draw the glass.The glass was then pulled into smaller lengths. The glass walls wereallowed to collapse and seal while at high temperature. This is how a 4mm length glass was constructed. The starting inner diameter of theglass tube was 3 mm. From this 3 mm ID glass, a piece of 4 mm in lengthwas successful drawn and ignited with RF energy. The electrodes at theend of the glass can be left as part of the glass containers or can beremoved. Additional heating was provided to anneal the various glassesto remove or minimize trapped stresses inside the structure. In somecases, metals wires, metal coils, Carbon Nano Tubes, Nano Magnets wereintroduced inside the glass containers through a lateral aperture.

Besides work with the above-noted gasses, forming gas (i.e., a mixtureof hydrogen up to 5.7% and nitrogen) was successfully tested.

In one embodiment of the invention, the sealed tubes were subjected to acleaning process to “burn” organic contaminants from the tubes. Thecleaning process involved an air plasma ignited and sustained with a 400milliamps, 12,000 volt, 350 EC, plasma treatment.

This experimental work demonstrated ignition of plasma (even insidephantoms to be discussed below) with the assistance of a Tesla Coil,power pulsing and/or modulation, electric and magnetic field gradientsand transients, CNT and metallic additives, and the above in combinationwith the presence of a magnetic field, especially a field from a MRI.Indeed, plasma operation in the gas containers inside the MRI have beensustained at power levels as low as 5 Watts.

Indeed, even when “phantoms” representing human blood were wrappedaround the quartz tubes, plasma ignition still occurred. Phantoms of athickness of about 2-15 cm have been tested successfully under differentRF frequencies and antenna designs. Temperature sensors in the phantomsshowed an acceptable level of heating of the phantom. Thus, in oneembodiment of the invention, plasma ignition and light generationtherefrom are possible in a human or animal body as the subject of lighttherapy or light treatments.

In other demonstrations, a RF frequency at 915 MHz was used to ignite aplasma inside container separated from the RF antenna by a phantom of athickness about 2.5 cm. In that demonstration, the gas containers werebuilt as described before.

One typical phantom recipe contains (by weight); 70% laboratory gradeethylene glycol, 28% distilled water and 2% noniodized table salt.Tissue equivalent phantoms for performing power deposition specificabsorption rate (SAR) studies of RF and microwave sources have beenconstructed from numerous materials. For example, even solid gelledphantoms have been used. The Table below describes the properties ofvarious phantom mixtures.

Weight Percentage Components for Liquid and Solid Phantom Models ofHuman Liver Tissue at 915 MHz.

Phantom Desired components properties Mixture 1 Mixture 2 Mixture 3Mixture 4 Mixture 5 Liquid phantoms *** Water 4.93 8.89 28 28.5 44.54Ethylene Glycol 93.9 90 70.5 69.85 54.1 NaCl 1.17 1.11 1.5 1.65 1.36Dielectric constant 55 ± 6  33.7 39.5 49.1 51.0 57.3 Conductivity (S/m)1.0 ± 0.2 0.93 1.05 1.02 0.99 1.28 Solid phantoms *** Water 51.02 52.9651.6 52.4 Sugar 46.01 43.88 46.56 45 NaCl 0.82 1.02 1.24 1.4 HEC *5000,**3400 2.05* 2.04** 0.52* 1.0 Dowicil 75 0.1 0.1 0.1 0.1 Dielectricconstant 55 ± 6  51.3 51.4 52.0 54.7 Conductivity (S/m) 1.0 ± 0.2 0.961.02 1.13 1.38 More solid More liquid Muscle (6) *HEC 5000; **HEC 3400;*** Bold = preferred mixtures

The following papers incorporated herein by reference in their entiretyprovide descriptions of phantoms: 1) Chou C K, Chen G, Guy A W, Luk K H.Formulas for preparing phantom muscle tissue at variousradiofrequencies. Bioelectromag. 1984; 5:435-41; 2) Hartsgrove G,Kraszewski A, Surowiec A. Simulated biological materials forelectromagnetic radiation absorption studies. Bioelectromag. 1987;8:29-36; 3) Stauffer P R, Rossetto F, Prakash M, Neuman D G, Lee T.Phantom and animal tissues for modelling the electrical properties ofhuman liver. Int J Hyperthermia. 2003; 19(1):89-101; and 4) Neuman D G,Stauffer P R, Jacobsen S, Rossetto F. SAR pattern perturbations fromresonance effects in water bolus layers used with superficial microwavehyperthermia applicators. Int J Hyperthermia. 2002; 18(3):180-93.

In one demonstration, a SigmaEye pelvic applicator was used to activatevarious gas containers having a small electrode with RF excitation whenthe gas container was positioned in the middle of a 15 cm diametersaline phantom load inside a full waterbolus inside the SigmaEye pelvicapplicator. The gas container in this demonstration was more or lesscentered inside the SigmaEye applicator which is an oval (eye) shape of47×56 cm so the gas container was located deep in water load as well asin the saline (body) load. A discussion of various applicators(including the SigmaEye applicator) is given below.

In one embodiment, the RF or microwave power applied is applied at onepower for plasma ignition then at a lower power for plasma maintenance.

In one embodiment the plasma ignition is achieved through a Tesla coilcapable of producing a high voltage gradient around its antenna.Bringing the Tesla coil in proximity or in contact with the glasscontainer produced ignition. The plasma is then sustained using RFenergy in the presence or absence of a magnetic field.

Alternatively, other mechanisms for ionization such as ionization in thegas container up converter by x-rays or high energy particles can beused to ignite the plasma. Alternatively, other mechanisms forionization such as the application of energy from a Tesla coil can beused to ignite the plasma.

In one demonstration of the invention, a 140 MHz phased array of dipoleantennas has been used to couple power through a phantom. FIG. 78A is aphotographic depiction of a phased array of dipole antennas surroundinga phantom.

In another demonstration, a single dipole antenna operated at 140 MHzignited and sustained a plasma inside a phantom at a depth of 6 cm. Inthis demonstration, the array delivered a power of 200 W to 50 W to gascontainers located 10 cm from the array. A phantom covered the gascontainers.

In one embodiment of the invention, the RF or microwave power applied isapplied in a duty cycle to reduce the heating of the medium in which thegas container up converters are disposed. In one embodiment, the RF ormicrowave power applied is applied with a phased array of antennas toreduce the overall heating of the medium in which the gas container upconverters are disposed while increasing the field strength locally at aposition inside the medium where the emitted light is need to induce achange in the medium.

In particular, a Spin Echo pulse sequence has been used to demonstratethe ability to activate gas ionization and plasma generation andsustainment with only the RF coils in the MRI bore, which emit veryshort RF pulses during MRI pulse sequences to excite the proton spins.Using spin echo pulse sequences, which feature the highest power pulsesachievable with commercial pulse sequences, gases in millimeter sizequartz tubes in a phantom were ignited at the frequency of the RFpulses. This was performed using the RF body coil and the quadraturetransmit/receive head coil, both within the clinical specific absorptionrate (SAR) limits. Better ignition could be achieved with customizedpulse sequences with longer RF pulse duration. Up to 1.4 Kilowatt pulsescould be applied, without excessively heating the phantom. The pulsefrequency was changed from 1000 milliseconds to 500 ms, 250 ms, 100 ms,50 ms and 35 ms.

Frequency Hopping has been demonstrated to activate plasma emission ingas containers at a lower power than otherwise possible. In this mode ofoperation, the operational frequency is switched between a first andsecond frequency regime (both of which show a good match (minimumimpedance mismatch). By rapidly switching frequencies from one frequencyregime leading to another frequency regime of good match lower powerplasma emission was demonstrated. Moreover, this effect was enhanced inthe presence of a magnetic field (especially near or inside an MRI).

High Power Pulse Modulation by way of a power-modulated signal with veryhigh power and very short pulse width is a way to generate high fieldstrengths with sufficiently low average power to activate plasmaemission without over-heating tissue. Such pulse modulation techniquescould work on any antenna design.

Flux transients demonstrate the ability to activate plasma emission at alower power than otherwise possible. By rapidly moving the plasmacontainer through the field or physically tapping the lamp, fluxtransients have demonstrated plasma emission at a lower power thanotherwise possible. In one demonstration, when a conductive loop builtinto a gas container was passed through an electromagnetic field, itsincreased energy coupling lead to plasma ignition.

Phase Shifting/Switching demonstrate the ability to activate florescencewith lower power level than otherwise possible by rapidly switchingphase between adjacent or opposing antennas.

X-Ray assistance has demonstrate that, when inner walls of the gascontainers are coated with a material that would generate secondaryelectrons upon X-Ray exposure, the secondary electrons enter into highenergy excitations due to RF and/or MW energy, thereby producing lowerpower plasma ignitions. Higher energy excitations are possible in thepresence of a magnetic field.

In one embodiment of the invention, free-standing microwave and rfreceptors can be used to receive incident electromagnetic radiation(transmitted through an optically opaque medium, such as biologicaland/or human tissue) and generate visible or ultraviolet light. Indeed,in one embodiment of the invention, the wavelength of light generated isdetermined by the gas (or gasses) in the receptors. Moreover, in oneembodiment of the invention, the use of one or more of gasses such ashydrogen, argon, nitrogen, xenon, ammonia, iodine vapor; mercury vapor;an organic gas, and hydrogen-nitrogen mixtures, and/or mixtures thereofnot only serve to “tune” the wavelength, but are considered ofassistance (especially the low ionization potential gasses such asiodine vapor; mercury vapor; and organic gasses) for ignition of theplasma. Low ionization materials such as sodium and barium strontiumoxide have shown a propensity for assisting in plasma initiation andmaintenance.

Moreover, in one embodiment of the invention, the gas container caninclude structures which provide a source of electrons (from electricfield induced emission, for example) into the gas of the containment toassist in ionization. Thus, the gas container can include at least oneof a carbon structure, a carbon nanotube, a single wall carbon nanotube,a double wall carbon nanotube, grapheme, and metal materials made ofaluminum or copper.

This work has realized that macroscopic and microscopic gas containingupconverter structures can be used in various applications andparticularly medical applications for light therapy or light treatmentsinside a living animal or person.

In one example, macroscopic or a plurality of microscopic gas containingup converter structures of the invention can be mounted on catheters forinsertion into a patient. Catheters have been and are widely used inmedical applications. Catheters have been particularly useful intreating for example enlarged prostates by microwave treatment. In thismedical application, a catheter is inserted into the urethra of the manto be treated until an inflatable balloon, which is located at the frontinsertion end of the catheter, is positioned in the urinary bladder. Theballoon is then inflated and held stationary within the bladder.Subsequently, in this prior microwave treatment, a microwave antenna wasinserted through an inner lumen of the catheter until it is locatedadjacent to the prostate. The antenna was arranged at the front end ofan antenna cable, while the other end of the cable, which protruded fromthe catheter, was connected to a microwave energy source.

Here, the need to internally supply microwave power through the innerlumen of the catheter imposes restrictions on the catheter, the spacewithin the catheter, and the power transfer to the end of the catheter.Furthermore, any stray microwave radiation would locally heat theprostate. Catheters for the conventional microwave treatment of prostatefrequently used a catheter tube made of polyvinylchloride (PVC) orpolytetrafluoroethylene (PTFE). Such catheters are highly flexible andcan form the basis for the catheter of this embodiment of the invention.Typically, a catheter tube has a wall thickness of between 0.1 and 0.3mm. The outer catheter layer can be made microporous PTFE which has goodpadding properties. This is advantageous when the catheter is movedthrough bends of the body such as the urethra. Furthermore, microporousPTFE has very good sliding properties.

The outer layer of the catheter of this invention can be made from atape of microporous PTFE which is wrapped around the carrier tube, or aseparate tube of microporous PTFE which is applied over the carrier tubeor can be extruded onto the carrier tube, either simultaneously orsubsequently.

FIG. 78B is a schematic of catheter 51 of the invention having a gascontainer upconverter 57 at or near the distal end of the catheter. Atthe end of the catheter which is inserted first, there can be disposedan inflatable balloon 53 which is shown in the inflated state in FIG. 78. At the end of the catheter 51 opposite to the insertion end, the gascontainer upconverter 57 is disposed. Cooling water tubes 59 and sensorlines 61 can also be also disposed in the catheter 51.

In this arrangement, the gas container upconverter 57 can be positionedinside the human body in a vicinity of the organ to be treated. A humanperson having the catheter with gas container upconverter 57 in placecan then (or beforehand) be positioned in an NMR unit, as describedabove. Powering of the NMR then activates the ionizable gas in gascontainer upconverter 57 producing UV or visible light for phototherapyor light treatments of the organ. Appropriate phototherapies aredescribed in U.S. patent application Ser. No. 12/389,946,PCT/US2009/050514 application, U.S. provisional application 61/171,158,U.S. patent application Ser. No. 12/417,779, U.S. patent applicationSer. No. 12/725,108, the entire contents of which are incorporatedherein by reference. A discussion of various phototherapies useful inthis invention by way of light from gas containing upconverterstructures of this invention is included below.

In general, numerous microwave and RF applicators have been demonstratedby one or more of the inventors. Microwave applicators operating atfrequencies like 433 and 915 MHz typically heat superficial tissueregions within about 3-4 cm of skin surface. Thus, a rapidly attenuatingfield penetrates somewhat deeper, but the primary field and thuseffective heating is limited to about 3-4 cm. Radiofrequency fields fromabout 70-200 MHz have much longer wavelength and can penetrate deeperinto tissue under an antenna. While still attenuating with depth, it ispossible to obtain a local maximum (focal hot spot) as deep as the bodyaxis by aiming multiple antennas with correct phase relationship to havefields add at depth. In one embodiment of the invention, microwave andRF applicators as discussed above and elaborated on below can be used inthe invention to excite the gasses in the gas containing upconverterstructures of the invention.

Of interest here are applicators already available from hyperthermiamedical treatment apparatus. The following papers incorporated herein byreference in their entirety provide descriptions of applicators suitablefor the invention and provide descriptions of their configuration andoperating frequencies: 1) Lee E R. Electromagnetic superficial heatingtechnology. In: Seegenschmiedt M H, Fessenden P, Vernon C C, editors.Thermo-radiotherapy and Thermo-chemotherapy. Berlin, Heidelberg:Springer-Verlag; 1995. p. 193-217; 2) Hand J W, Hind A J. A review ofmicrowave and R F applicators for localized hyperthermia. In: Hand J W,James J R, editors. Physical Techniques in Clinical Hyperthermia.Letchworth, Hertfordshire, England: Research Studies Press; 1986. p.98-148; 3) Stauffer P R. Thermal therapy techniques for skin andsuperficial tissue disease. In: Ryan T P, editor. A critical review,matching the energy source to the clinical need. Bellingham W A: SPIEOptical Engineering Press; 2000. p. 327-67; 4) Stauffer P R. Evolvingtechnology for thermal therapy of cancer. Int J Hyperthermia. 2005;21(8):731-44; 5) Stauffer P R, Diederich C J, Pouliot J. Thermal therapyfor cancer. In: Thomadsen B, Rivard M, Butler W, editors. BrachytherapyPhysics, Second Edition, Joint AAPM/ABS Summer School, Med PhysMonograph No 312005. p. 901-32; 6) Sneed P K, Stauffer P R, Li G, Sun X,Myerson R. Hyperthermia. In: Phillips T, Hoppe R, Roach M, editors.Textbook of Radiation Oncology Third Edition. Philadelphia: ElsevierSaunders Co; 2010. p. 1564-93.

For both radiofrequency (RF) and microwave (MW) radiation, absorbedpower density decreases exponentially with depth in tissue. In order toselect the optimum frequency of EM field for depositing energy in atumor, the critical factors are tumor size and depth below the tissuesurface relative to EM wavelength, and proximity to adjacent criticalnormal tissue structures. For the practical range of frequencies used inhyperthermia and applicable here in the invention for plasma excitationfrom 1-1000 MHz, the wavelengths in soft tissue vary from about 4.5 cmat 1000 MHz up to 2 m at the lower RF frequencies. The maximum spatialresolution of power deposition (focal spot size) is approximately onehalf this wavelength. The effective heating depth may decrease furtheras a result of power deposition peaks in the spatially complex antennanear field, and heterogeneities of tissue properties which increasereflection and refraction perturbations of the EM field at tissueinterfaces. In general, it may be expected that the upper microwavefrequencies may be expected to provide localized heating of skin andsurface tissues while the lower RF frequencies will heat larger anddeeper regions of the body.

Microwave waveguide: The most basic EM applicator used for heatingsuperficial tissue is the microwave waveguide with single linearlypolarized monopole feed. Aperture size is generally designed with oneside at least a half wavelength long. The interior is often filled orlined with high dielectric constant material to reduce the effectivewavelength in the waveguide structure. Electromagnetic horn applicatorsare a close variant of the waveguide applicator, with tapered openingsto control the divergence of radiated field. In general, horns providesomewhat larger effective field size than equivalent size waveguides.Flared horns with the two sides parallel to the electric field replacedwith low ϵr Lucite to expand the SAR distribution in the H-plane havebeen used. A six (6) element array of Lucite Cone Applicators (LCA) hasdemonstrated uniformity of heating. The LCA applicators have been usedin up to 3H2 arrays, treating surface areas up to 600 cm². The followingpapers incorporated herein by reference in their entirety providedescriptions of microwave waveguides suitable for the invention andprovide descriptions of their configuration and operatingfrequencies: 1) Rietveld P J M, Van Putten W L J, Van Der Zee J, VanRhoon G C. Comparison of the clinical effectiveness of the 433 MHzLucite cone applicator with that of a conventional waveguide applicatorin applications of superficial hyperthermia. International Journal ofRadiation Oncology Biology Physics. 1999; 43(3):681-7; 2) Van Rhoon G C,Rietveld P J M, Van Der Zee J. A 433 MHz Lucite cone waveguideapplicator for superficial hyperthermia. Int J Hyperthermia. 1998;14(1):13-27′ 3) Chan K W, McDougall J A, Chou C K. FDTD simulations ofClini-Therm applicators on inhomogeneous planar tissue models. Int JHyperthermia. 1995; 11(6):809-20; 4) Straube W L, Myerson R J, Emami B,Leybovich L B. SAR patterns of external 915 MHz microwave applicators.Int J Hyperthermia. 1990; 6(3):665-70; 5) Turner P F, Kumar L. Computersolution for applicator heating patterns. National Cancer InstituteMonograph. 1982; 61:521-3.

Conformal Antennas—For heating large areas of superficial disease suchas chest wall recurrence of breast carcinoma, large multi-elementmicrowave arrays are generally preferred to uniformly cover largecontoured regions of the torso. Examples include the Dual ConcentricConductor based Conformal Microwave Array (CMA) which was tested in thispreliminary exercise. Heating is typically <2-3 cm depth. Anotherexample is a 915 MHz sixteen (16) element planar waveguide arrayapplicator Microtherm 1000 (Labthermics Technologies Corp., ChampaignIll.) which was shown suitable for treating superficial tissue regionsup to 13H13H1.5 cm. Another array heating approach makes use ofinductive loop coupled Current Sheet Applicators (CSA) which are smaller(7.3H5.9H3.3 cm) and lighter in weight than typical waveguideapplicators and can be connected together in hinged flexible arrays forcontoured surfaces A 433 MHz four element CSA array demonstrated moreuniform and higher overall temperature distributions than possible withearlier devices, with tumor heating temperatures of 41.0±1.5° C. and42.2±1.4° C., respectively obtained.

Another example is a printed circuit board (PCB) based microstripantenna technology have received attention due to the ability to formalmost arbitrarily large arrays from relatively low cost, lightweightand flexible PCB material. Microstrip patches, slot apertures, andspiral microstrip antennas have been used. Microstrip applicators appearbest suited to tumors that extend up to and include the tissue surfacerather than those located beneath a layer of high resistivity fat.Contact Flexible Microstrip Applicators (CFMA) are available in severaldifferent sizes that can be used at frequencies ranging from 40 MHz to915 MHz. The applicators have been shown to produce large effectivefield sizes up to 400 cm² with relatively uniform SAR patterns

Conformal Microwave Array (CMA) applicators consisting of an array ofsquare radiating apertures etched from a single layer of flexible copperfoil and driven non-coherently at 915 MHz have been used. Subsequently,radiation patterns from the square annular slot Dual ConcentricConductor (DCC) apertures were analyzed theoretically with FiniteDifference Time Domain (FDTD) simulations for a variety of aperturesizes and design configurations, and the simulations verified withmeasurements of SAR in muscle equivalent phantoms.

The following papers incorporated herein by reference in their entiretyprovide descriptions of conformal applicators suitable for the inventionand provide descriptions of their configuration and operatingfrequencies: 1) Gelvich E A, Mazokhin V N. Contact flexible microstripapplicators (CFMA) in a range from microwaves up to short waves. IEEETrans Biomed Eng. 2002; 49:1015-23; 2) Lee E R, Wilsey T R,Tarczy-Hornoch P, Kapp D S, Fessenden P, Lohrbach A W, et al. Bodyconformable 915 MHz microstrip array applicators for large surface areahyperthermia. IEEE Trans Biomed Eng. 1992; 39(5):470-83; and 3) StaufferP, Maccarini P, Arunachalam K, Craciunescu O, Diederich C, Juang T, etal. Conformal microwave array (CMA) applicators for hyperthermia ofdiffuse chest wall recurrence. Int J Hyperthermia. 2010; 26(7):686-98.

Another device that can deposit energy deep in the body with a singleexternal power source is the Coaxial TEM applicator. This deviceconsists of a coaxial cable like structure that is large enough to placethe entire patient inside a hollow 60 cm diameter “inner conductor”chamber that is filled with coupling water. With only a single 70 MHzpower generator to produce an axially directed electric field, partialsteering of the SAR around the body cross section is possible byshifting patient position within the 60 cm aperture cross section. Sinceit is desirable to both penetrate deep in the body and restrict heatingto specific tumor containing regions at depth, there have been a numberof electromagnetic radiating array applicators developed which aredesigned to steer energy deposition within the body. One such device isthe four wave guide array or Matched Phased Array (MPA) system whichallows custom positioning of waveguide sources on the patient surfaceaccompanied by phase and amplitude adjustments of all four sources tosteer power deposition at depth. This device has demonstrated theability to generate low to moderate temperatures (40-41° C.) in deeptumors in clinical studies since 1987.

Radiofrequency Phased-Array-Deep heating antenna arrays have beenconstructed from concentric ring arrays of dipole radiators mounted on aplexiglass cylinder or elliptical shape form. Arrays with 8 dipolesconnected in pairs to four RF power amplifiers have been constructed inannular phased arrays for arms, legs and pelvis and more recently intoMagnetic Resonance Thermal Imaging compatible arrays with one ring orthree rings of 4 dipole pairs. In one example, an Annular Phased ArraySystem (APAS) having 4 amplifiers driving 8 dipole antennas positionedin a fixed pattern around the patient circumference and coupled withdeionized water bolus has been developed by BSD Medical Corp. Subsequentdevelopment produced the Sigma-60 applicator operating providingincreased flexibility of control from four independent phase andamplitude controls for the 8 dipoles as well as a more patient friendlyinterface, as seen in FIG. 15 . Improved localization has been reportedfor this device as well as clinical utility in a number of deep tissuesites. BSD Medical Corp extended its product line with a new series ofSigma-Eye applicators operating at 100 MHz, which provide axial as wellas lateral steering of power deposition with three rings of 8 dipoleantennas each. This later configuration has sufficient adjustabilitythat an MRI-compatible heat applicator system along with an MRI magnetthat facilitates pre-treatment planning scans of the patient in theintended treatment configuration. Moreover, associated software isavailable to non-invasively monitor deep tissue temperature andphysiologic changes during heat treatment is available.

In one embodiment of the invention, the temperature surrounding the gascontainers can be noninvasively measured using magnetic resonancethermometry (MRT), which can produce 2D images of the temperaturechanges in the tissue surrounding the lamps. Several methods have beendeveloped for performing MRT in vivo, which can then be used todetermine the heat distribution in the body caused by RF and argon tubeheating. These methods can be applied to a number of differentapplicators and regions of the body. T The following papers incorporatedherein by reference in their entirety provide descriptions of magneticresonance thermometry (MRT) suitable for the invention: 1) Carter, D.L., J. R. MacFall, S. T. Clegg, X. Wan, D. M. Prescott, H. C. Charles,and T. V. Samulski, Magnetic resonance thermometry during hyperthermiafor human high-grade sarcoma. Int J Radiat Oncol Biol Phys, 1998. 40(4):p. 815-22; 2) Wyatt C R., Soher, B J., Maccarrini, P., Stauffer, P.,MacFall, J R. Hyperthermia MRI Temperature Measurement: Evaluation ofMeasurement Stabilization Strategies for Extremity and Breast Tumors.International Journal of Hyperthermia, 25(6): 422-433.DOI:10.1080/02656730903133762.

The following papers incorporated herein by reference in their entiretyprovide descriptions of phased array applicators suitable for theinvention and provide descriptions of their configuration and operatingfrequencies: 1) Wust P, Beck R, Berger J, Fahling H, Seebass M,Wlodarczyk W, et al. Electric field distributions in a phased-arrayapplicator with 12 channels: Measurements and numerical simulations. MedPhys. 2000; 27(11):2565-79; 2) Turner P, Schaefermeyer T, editors. SigmaEye EM phased array and the BSD-2000 3D system. 16th Annual Meeting ofthe European Society for Hyperthermic Oncolgy; 1999; Berlin: HumboltUniversity; 3) Kato H, Uchida N, Kasai T, Ishida T. A new applicatorutilizing distributed electrodes for hyperthermia: theoretical approach.Int J Hyperthermia. 1995; 11(2):287-94; and 4) Kato H, Hand J W, MichaelM V, Furukawa M, Yamamoto O, Ishida T. Control of specific absorptionrate distribution using capacitive electrodes and inductiveaperture-type applicators: implications for radiofrequency hyperthermia.IEEE Trans Biomed Eng. 1991; 38(7):644.

In this invention, these applicators (developed for hyperthermia) areusable to excite plasmas in the gas containing upconverter structures ofthe invention, thereby providing the capability to leverage thispre-existing technology base to provide photodynamic therapy in additionto, in conjunction with, or separate from a hyperthermia treatment.

A programmed Sigma-Eye applicator has been used with multiple antennasplaced concentrically around a tissue load or phantom with the gascontaining upconverter structures of the invention placed inside. Thefields from each antenna are combined and there are regions ofconstructive phase addition and regions of destructive interference. Thearray is considered focused where the fields add constructively toproduce a local maximum. In the center of a perfectly circular arraywith N antennas of equal power and phase, the field in the central focusis N2 as much as it would be from one antenna alone. If the phase anglesare shifted appropriately to launch the wave from some antennas laterthan from other antennas, then the local field maximum will be shiftedcloser to the antennas with phase delay. By rapidly shifting therelative phase of all antennas between fixed patterns that produce localmaximums in different locations of the central tissue load, the hot spotcan be shifted around inside the tissue volume allowing higher power andfield strengths but spreading the average power and heating around alarger volume. This effect was seen in the ability to selectively igniteplasmas in separate gas containers in separate regions of the phantom.Plasma emission can thus be achieved over larger areas for same increasein temperature.

In one embodiment of the invention, a Meta-material Lens Applicator canbe used. This kind of applicator represents a new class of metamaterialantennas with great potential to increase effective penetration and evenproduce a minor focus of microwave energy at depth. The technology hasdemonstrated effective fields at depth using convenient low profilelightweight and power efficient antennas driven at 433 and 915 MHz.Maximum penetration and ability to phase focus is not yet determined butmay increase to 4-6 cm at 433-915 MHz and more with phase addition ofmultiple antenna arrays. These antennas are described by Maccarini P,Aknine G, Wyatt C, Stauffer: P. in Characterization of the FirstConformal Metamaterial Lens Applicator (CMLA) for Hyperthermia, EuropeanSociety Hyperthermic Oncology; Rotterdam 2010, the entire contents ofwhich are incorporated herein by reference.

In one embodiment of the invention, a parabolic antenna could be used toproduce a localized high intensity region for plasma ignition in the gascontaining upconverter structures of the invention.

Photodynamic Therapy (PDT)

PDT is a relatively new light-based treatment, which has recently beenapproved by the United States Food & Drug Administration (FDA) for thetreatment of both early and late-stage lung cancer. Other countries haveapproved PDT for treatment of various cancers as well. Unlikechemotherapy, radiation, and surgery, PDT is useful in treating all celltypes, whether small cell or non-small cell carcinoma. PDT involvestreatment of diseases such as cancer using light action on a specialphotoactive class of drugs, by photodynamic action in vivo to destroy ormodify tissue [Dougherty T. J. and Levy J. G., “Photodynamic Therapy andClinical Applications”, in Biomedical Photonics Handbook, Vo-Dinh T.,Ed., CRC Press, Boca Raton Fla. (2003)]. PDT, which was originallydeveloped for treatment of various cancers, has now been used to includetreatment of pre-cancerous conditions, e.g. actinic keratoses,high-grade dysplasia in Barrett's esophagus, and non-cancerousconditions, e.g. various eye diseases, e.g. age related maculardegeneration (AMD). Photodynamic therapy (PDT) is approved forcommercialization worldwide both for various cancers (lung, esophagus)and for AMD.

The PDT process requires three elements: (1) a PA drug (i.e.,photosensitizer), (2) light that can excite the photosensitizer and (3)endogenous oxygen. The putative cytotoxic agent is singlet oxygen, anelectronically excited state of ground state triplet oxygen formedaccording to the Type II photochemical process, as follows.PA+hν→ ¹PA*(S) Excitation¹PA*(S)→³PA*(T) Intersystem crossing for singlet to triplet state³PA*(T)+O₂→¹O*₂+PA Energy transfer from the drug to singlet oxygenwhere PA=photo-active drug at the ground state; ¹PA*(S)=excited singletstate; ³PA*(T)=excited triplet state; ¹O*₂=singlet excited state ofoxygen

Because the triplet state has a relatively long lifetime (μsec toseconds) only photosensitizers that undergo efficient intersystemcrossing to the excited triplet state will have sufficient time forcollision with oxygen in order to produce singlet oxygen. The energydifference between ground state and singlet oxygen is 94.2 kJ/mol andcorresponds to a transition in the near-infrared at 1270 nm. Most PAphotosensitizers in clinical use have triplet quantum yields in therange of 40-60% with the singlet oxygen yield being slightly lower.Competing processes include loss of energy by deactivation to groundstate by fluorescence or internal conversion (loss of energy to theenvironment or surrounding medium).

However, while a high yield of singlet oxygen is desirable it is by nomeans sufficient for a photosensitizer to be clinically useful.Pharmacokinetics, pharmacodynamics, stability in vivo and acceptabletoxicity play critical roles as well [Henderson B W, Gollnick S O,“Mechanistic Principles of Photodynamic Therapy”, in BiomedicalPhotonics Handbook, Vo Dinh T, Ed., CRC Press, Boca Raton Fla. (2003)].For example, it is desirable to have relatively selective uptake in thetumor or other tissue being treated relative to the normal tissue thatnecessarily will be exposed to the exciting light as well.Pharmacodynamic issues such as the subcellular localization of thephotosensitizer may be important as certain organelles appear to be moresensitive to PDT damage than others (e.g. the mitochondria). Toxicitycan become an issue if high doses of photosensitizer are necessary inorder to obtain a complete response to treatment. An important mechanismassociated with PDT drug activity involves apoptosis in cells. Uponabsorption of light, the photosensitiser (PS) initiates chemicalreactions that lead to the direct or indirect production of cytotoxicspecies such as radicals and singlet oxygen. The reaction of thecytotoxic species with subcellular organelles and macromolecules(proteins, DNA, etc) lead to apoptosis and/or necrosis of the cellshosting the PDT drug. The preferential accumulation of PDT drugmolecules in cancer cells combined with the localized delivery of lightto the tumor, results in the selective destruction of the cancerouslesion. Compared to other traditional anticancer therapies, PDT does notinvolve generalized destruction of healthy cells. In addition to directcell killing, PDT can also act on the vasculature, reducing blood flowto the tumor causing its necrosis. In particular cases it can be used asa less invasive alternative to surgery.

There are several chemical species used for PDT includingporphyrin-based sensitizers. A purified hematoporphyrin derivative,Photofrin®, has received approval of the US Food and DrugAdministration. Porphyrins are generally used for tumors on or justunder the skin or on the lining of internal organs or cavities becausetheses drug molecules absorbs light shorter than 640 nm in wavelength.For tumors occurring deep in tissue, second generation sensitizers,which have absorbance in the NIR region, such as porphyrin-based systems[R. K. Pandey, “Synthetic Strategies in designing Porphyrin-BasedPhotosensitizers’, in Biomedical Photonics Handbook, Vo-Dinh T., Ed.,CRC Press, Boca Raton Fla. (2003)], chlorines, phthalocyanine, andnaphthalocyanine have been investigated.

PDT retains several photosensitizers in tumors for a longer time than innormal tissues, thus offering potential improvement in treatmentselectivity. See Comer C., “Determination of [3H]- and [14C]hematoporphyrin derivative distribution in malignant and normal tissue,”Cancer Res 1979, 3 9: 146-15 1; Young S W, et al., “Lutetium texaphyrin(PCI-0123) a near-infrared, water-soluble photosensitizer,” PhotochemPhotobiol 1996, 63:892-897; and Berenbaum M C, et al.,“Meso-Tetra(hydroxyphenyl)porphyrins, a new class of potent tumorphotosensitisers with favorable selectivity,” Br J Cancer 1986,54:717-725. Photodynamic therapy uses light of a specific wavelength toactivate the photosensitizing agent. Various light sources have beendeveloped for PDT, which include dye lasers and diode lasers. Lightgenerated by lasers can be coupled to optical fibers that allow thelight to be transmitted to the desired site. See Pass 1-11,“Photodynamic therapy in oncology: mechanisms and clinical use,” J NatlCancer Inst 1993, 85:443-456. According to researchers, the cytotoxiceffect of PDT is the result of photooxidation reactions, as disclosed inFoote C S, “Mechanisms of photooxygenation,” Proa Clin Biol Res 1984,170:3-18. Light causes excitation of the photosensitizer, in thepresence of oxygen, to produce various toxic species, such as singletoxygen and hydroxyl radicals. It is not clear that direct damage to DNAis a major effect; therefore, this may indicate that photoactivation ofDNA crosslinking is not stimulated efficiently.

Photoactivation Treatments

For the treatment of cell proliferation disorders, an initiation energysource (e.g, light from the gas containing up converter structures ofthe invention) can provide an initiation energy that activates anactivatable pharmaceutical agent to treat target cells within a subject.In one embodiment, the initiation energy source is applied indirectly tothe activatable pharmaceutical agent, preferably in proximity to thetarget cells. Within the context of the present invention, the phrase“applied indirectly” (or variants of this phrase, such as “applyingindirectly”, “indirectly applies”, “indirectly applied”, “indirectlyapplying”, etc.), when referring to the application of the initiationenergy, means the penetration by the initiation energy into the subjectbeneath the surface of the subject and to the activatable pharmaceuticalagent within a subject.

Although not intending to be bound by any particular theory or beotherwise limited in any way, the following theoretical discussion ofscientific principles and definitions are provided to help the readergain an understanding and appreciation of the present invention. As usedherein, the term “subject” is not intended to be limited to humans, butmay also include animals, plants, or any suitable biological organism.

As used herein, the phrase “cell proliferation disorder” refers to anycondition where the growth rate of a population of cells is less than orgreater than a desired rate under a given physiological state andconditions. Although, preferably, the proliferation rate that would beof interest for treatment purposes is faster than a desired rate, slowerthan desired rate conditions may also be treated by methods of thepresent invention. Exemplary cell proliferation disorders may include,but are not limited to, cancer, bacterial infection, immune rejectionresponse of organ transplant, solid tumors, viral infection, autoimmunedisorders (such as arthritis, lupus, inflammatory bowel disease,Sjogrens syndrome, multiple sclerosis) or a combination thereof, as wellas aplastic conditions wherein cell proliferation is low relative tohealthy cells, such as aplastic anemia. Particularly preferred cellproliferation disorders for treatment using the present methods arecancer, Staphylococcus Aureus (particularly antibiotic resistant strainssuch as methicillin resistant Staphylococcus Aureus or MRSA), andautoimmune disorders.

As used herein, an “activatable pharmaceutical agent” (alternativelycalled a “photoactive agent” or PA) is an agent that normally exists inan inactive state in the absence of an activation signal. When the agentis activated by a matching activation signal under activatingconditions, it is capable of effecting the desired pharmacologicaleffect on a target cell (i.e. preferably a predetermined cellularchange).

Signals that may be used to activate a corresponding agent may include,but are not limited to, photons of specific wavelengths (e.g. x-rays, orvisible light), electromagnetic energy (e.g. radio or microwave),thermal energy, acoustic energy, or any combination thereof.

Activation of the agent may be as simple as delivering the signal to theagent or may further premise on a set of activation conditions. Forexample, in the former case, an activatable pharmaceutical agent, suchas a photosensitizer, may be activated by UV-A radiation (e.g, UV-Alight from the gas containing up converter structures of the invention).Once activated, the agent in its active-state may then directly proceedto effect a cellular change.

Where activation may further premise upon other conditions, meredelivery of the activation signal may not be sufficient to bring aboutthe desired cellular change. For example, a photoactive compound thatachieves its pharmaceutical effect by binding to certain cellularstructure in its active state may require physical proximity to thetarget cellular structure when the activation signal is delivered. Forsuch activatable agents, delivery of the activation signal undernon-activating conditions will not result in the desired pharmacologiceffect. Some examples of activating conditions may include, but are notlimited to, temperature, pH, location, state of the cell, presence orabsence of co-factors. Selection of an activatable pharmaceutical agentgreatly depends on a number of factors such as the desired cellularchange, the desired form of activation, as well as the physical andbiochemical constraints that may apply. Exemplary activatablepharmaceutical agents may include, but are not limited to, agents thatmay be activated by photonic (electromagnetic) energy, acoustic energy,chemical or enzymatic reactions, thermal energy, or any other suitableactivation mechanisms.

When activated, the activatable pharmaceutical agent may effect cellularchanges that include, but are not limited to, apoptosis, redirection ofmetabolic pathways, up-regulation of certain genes, down-regulation ofcertain genes, secretion of cytokines, alteration of cytokine receptorresponses, production of reactive oxygen species or combinationsthereof.

The mechanisms by which an activatable pharmaceutical agent may achieveits desired effect are not particularly limited. Such mechanisms mayinclude direct action on a predetermined target as well as indirectactions via alterations to the biochemical pathways. A preferred directaction mechanism is by binding the agent to a critical cellularstructure such as nuclear DNA, mRNA, rRNA, ribosome, mitochondrial DNA,or any other functionally important structures. Indirect mechanisms mayinclude releasing metabolites upon activation to interfere with normalmetabolic pathways, releasing chemical signals (e.g. agonists orantagonists) upon activation to alter the targeted cellular response,and other suitable biochemical or metabolic alterations.

The treatment can be by those methods described in U.S. application Ser.No. 11/935,655, filed Nov. 6, 2007 (incorporated by reference above), orby a modified version of a conventional treatment such as PDT, but usinga plasmonics-active agent to enhance the treatment by modifying orenhancing the applied energy or, in the case of using an energymodulation agent, modifying either the applied energy, the emittedenergy from the energy modulation agent, or both.

In one embodiment, the activatable pharmaceutical agent is capable ofchemically binding to the DNA or mitochondria at therapeuticallyeffective amount. In this embodiment, the activatable pharmaceuticalagent, preferably a photoactivatable agent, is exposed in situ to anactivating energy emitted from an energy modulation agent, which, inturn receives energy from an initiation energy source.

Suitable activatable agents include, but are not limited to, photoactiveagents, sono-active agents, thermo-active agents, andradio/microwave-active agents. An activatable agent may be a smallmolecule; a biological molecule such as a protein, a nucleic acid orlipid; a supramolecular assembly; a nanoparticle; a nanostructure, orcombinations thereof; or any other molecular entity having apharmaceutical activity once activated.

The activatable agent may be derived from a natural or synthetic origin.Any such molecular entity that may be activated by a suitable activationsignal source to effect a predetermined cellular change may beadvantageously employed in the present invention. Suitable photoactiveagents include, but are not limited to: psoralens and psoralenderivatives, pyrene cholesteryloleate, acridine, porphyrin, fluorescein,rhodamine, 16-diazorcortisone, ethidium, transition metal complexes ofbleomycin, transition metal complexes of deglycobleomycin,organoplatinum complexes, alloxazines such as 7,8-dimethyl-10-ribitylisoalloxazine (riboflavin), 7,8,10-trimethylisoalloxazine (lumiflavin),7,8-dimethylalloxazine (lumichrome), isoalloxazine-adenine dinucleotide(flavine adenine dinucleotide [FAD]), alloxazine mononucleotide (alsoknown as flavine mononucleotide [FMN] and riboflavine-5-phosphate),vitamin Ks, vitamin L, their metabolites and precursors, andnapththoquinones, naphthalenes, naphthols and their derivatives havingplanar molecular conformations, porphyrins, dyes such as neutral red,methylene blue, acridine, toluidines, flavine (acriflavinehydrochloride) and phenothiazine derivatives, coumarins, quinolones,quinones, and anthroquinones, aluminum (111) phthalocyaninetetrasulfonate, hematoporphyrin, and phthalocyanine, and compounds whichpreferentially adsorb to nucleic acids with little or no effect onproteins. The term “alloxazine” includes isoalloxazines.

Endogenously-based derivatives include synthetically derived analogs andhomologs of endogenous photoactivated molecules, which may have or lacklower (1 to 5 carbons) alkyl or halogen substituents of thephotosensitizers from which they are derived, and which preserve thefunction and substantial non-toxicity. Endogenous molecules areinherently non-toxic and may not yield toxic photoproducts afterphotoradiation.

Table 1 lists some photoactivatable molecules capable of beingphotoactivated to induce an auto vaccine effect.

SSET and TTET rate constants for bichromophoric peptides k_(SSET) (s⁻¹)R_(model) (Å) Compound λ_(ex) (nm) E_(SSET) k_(s) of donor (s⁻¹)k_(SSET) (s⁻¹) (Average) R₀ (Å) R (Å) (Average) E_(TTET) k_(TTET) (s⁻¹)1B 224 96.3 9.5 × 10³ 2.44 × 10⁸  1.87 × 10³ 14.7 9 9.5 266 95 1.8 × 10⁸2.5   5 × 10² 280 94 1.36 × 10⁸  1A 224 80 9.5 × 10⁶ 3.8 × 10⁷ 3.67 ×10⁷ 14.7 11.8 14.1 266 79 3.6 × 10⁷ 2 3.6 × 10² 280 79 3.6 × 10⁷ 2B 22477 9.5 × 10⁵ 3.1 × 10⁷  3.9 × 10⁷ 14.7 11.9 6.5 266 81 3.9 × 10⁷ 32 9.4× 10³ 280 83 4.7 × 10⁷ 2A 224 69 9.5 × 10⁵ 2.1 × 10⁷   3 × 10⁷ 14.7 12.28.1 74.3 5.7 × 10⁴ 266 80 3.7 × 10⁷ 280 77 3.2 × 10⁷

TABLE 2 Biocompatible, endogenous fluorophore emitters. Excitation Max.Emission Max. Endogenous Fluorophores (nm) (nm) Amino acids: Tryptophan280 350 Tyrosine 275 300 Phenylalanine 260 280 Structural Proteins:Coltagen 325, 360 400, 405 Elastin 290, 325 340, 400 Enzymes andCoenzymes: flavin adenine dinucleotide 450 535 reduced nicotinamidedinucelotide 290, 351 440, 460 reduced nicotinamide dinucelotidephosphate 336 464 Vitamins: Vitamins A 327 510 Vitamins K 335 480Vitamins D 390 480 Vitamins B₆ compounds: Pyridoxine 332, 340 400Pyridoxamine 335 400 Pyridoxal 330 385 Pyridoxic acid 315 425 Pyrictoxalphosphate  5′-330 400 Vitamin B₁₂ 275 305 Lipids: Phospholipids 436 540,560 Lipofuscin 340-395 540, 430-460 Ceroid 340-395 430-460, 540Porphyrins 400-450 630, 690

The nature of the predetermined cellular change will depend on thedesired pharmaceutical outcome. Exemplary cellular changes may include,but are not limited to, apoptosis, necrosis, up-regulation of certaingenes, down-regulation of certain genes, secretion of cytokines,alteration of cytokine receptor responses, or a combination thereof.

Energy from light emitted from the gas containing up converterstructures of the invention may be transferred from one molecule toanother (intermolecular transfer) or from one part of a molecule toanother part of the same molecule (intramolecular transfer). Forexample, the receives electromagnetic energy may be converted intothermal energy. Energy transfer processes are also referred to asmolecular excitation.

Additionally, energy modulation agents may be included in the medium tobe treated. The energy modulation agents may upon receiving of lightfrom the gas containing up converter structures re-emit a light specificto a desired photo-driven reaction. Energy modulation agents (reactingto the light from the gas containing up converter structures) can have avery short energy retention time (on the order of fs-ns, e.g.fluorescent molecules) whereas others may have a very long half-life (onthe order of seconds to hours, e.g. luminescent inorganic molecules orphosphorescent molecules). Suitable energy modulation agents include,but are not limited to, a biocompatible metal nanoparticle, metal coatedwith a biocompatible outer layer, a chemiluminescent molecule whose rateof luminescence is increased by microwave activation, fluorescing dyemolecule, gold nanoparticle, a water soluble quantum dot encapsulated bypolyamidoamine dendrimers, a luciferase, a biocompatible phosphorescentmolecule, a biocompatible fluorescent molecule, a biocompatiblescattering molecule, a combined electromagnetic energy harvestermolecule, and a lanthanide chelate capable of intense luminescence.Various exemplary uses of these are described below in preferredembodiments.

The modulation agents may further be coupled to a carrier for cellulartargeting purposes. For example, a biocompatible molecule, such as afluorescing metal nanoparticle or fluorescing dye molecule that emits inthe UV-A band, may be selected as the energy modulation agent.

The energy modulation agent or the gas containing up converterstructures of the invention may be preferably directed to the desiredsite (e.g. a tumor) by systemic administration to a subject. Forexample, a UV-A emitting energy modulation agent may be concentrated inthe tumor site by physical insertion or by conjugating the UV-A emittingenergy modulation agent with a tumor specific carrier, such as anantibody, nucleic acid, peptide, a lipid, chitin or chitin-derivative, achelate, a surface cell receptor, molecular imprints, aptamers, or otherfunctionalized carrier that is capable of concentrating the UV-Aemitting source in a specific target tumor.

Additionally, the energy modulation agent can be used alone or as aseries of two or more energy modulation agents wherein the energymodulation agents provide an energy cascade from the light of the gascontaining up converter structures. Thus, the first energy modulationagent in the cascade will absorb the activation energy, convert it to adifferent energy which is then absorbed by the second energy modulationin the cascade, and so forth until the end of the cascade is reachedwith the final energy modulation agent in the cascade emitting theenergy necessary to activate the activatable pharmaceutical agent.

Although the activatable pharmaceutical agent and the energy modulationagent can be distinct and separate, it will be understood that the twoagents need not be independent and separate entities. In fact, the twoagents may be associated with each other via a number of differentconfigurations. Where the two agents are independent and separatelymovable from each other, they generally interact with each other viadiffusion and chance encounters within a common surrounding medium.Where the activatable pharmaceutical agent and the energy modulationagent are not separate, they may be combined into one single entity.

In general, photoactivatable agents may be stimulated by light of thegas containing up converter structures, leading to subsequentirradiation, resonance energy transfer, exciton migration, electroninjection, or chemical reaction, to an activated energy state that iscapable of effecting the predetermined cellular change desired. In a oneembodiment, the photoactivatable agent, upon activation, binds to DNA orRNA or other structures in a cell. The activated energy state of theagent is capable of causing damage to cells, inducing apoptosis. Themechanism of apoptosis is associated with an enhanced immune responsethat reduces the growth rate of cell proliferation disorders and mayshrink solid tumors, depending on the state of the patient's immunesystem, concentration of the agent in the tumor, sensitivity of theagent to stimulation, and length of stimulation.

A preferred method of treating a cell proliferation disorder of theinvention administers a photoactivatable agent to a patient, stimulatesthe photoactivatable agent by light of the gas containing up converterstructures to induce cell damage, and generates an auto vaccine effect.In one further preferred embodiment, the photoactivatable agent isstimulated via a resonance energy transfer.

One advantage is that multiple wavelengths of emitted radiation from thelight of the gas containing up converter structures may be used toselectively stimulate one or more photoactivatable agents or energymodulation agents capable of stimulating the one or morephotoactivatable agents. The energy modulation agent is preferablystimulated at a wavelength and energy that causes little or no damage tohealthy cells, with the energy from one or more energy modulation agentsbeing transferred, such as by Foerster Resonance Energy Transfer, to thephotoactivatable agents that damage the cell and cause the onset of thedesired cellular change, such as apoptosis of the cells.

Another advantage is that side effects can be greatly reduced bylimiting the production of free radicals, singlet oxygen, hydroxides andother highly reactive groups that are known to damage healthy cells.Furthermore, additional additives, such as antioxidants, may be used tofurther reduce undesired effects of irradiation.

Resonance Energy Transfer (RET) is an energy transfer mechanism betweentwo molecules having overlapping emission and absorption bands.Electromagnetic emitters are capable of converting an arrivingwavelength to a longer wavelength. For example, UV-B energy absorbed bya first molecule may be transferred by a dipole-dipole interaction to aUV-A-emitting molecule in close proximity to the UV-B-absorbingmolecule. Alternatively, a material absorbing a shorter wavelength maybe chosen to provide RET to a non-emitting molecule that has anoverlapping absorption band with the transferring molecule's emissionband. Alternatively, phosphorescence, chemiluminescence, orbioluminescence may be used to transfer energy to a photoactivatablemolecule.

In another embodiment, the invention includes the administration of theactivatable pharmaceutical agent, along with administration of a sourceof chemical energy such as chemiluminescence, phosphorescence orbioluminescence. The source of chemical energy can be a chemicalreaction between two or more compounds, or can be induced by activatinga chemiluminescent, phosphorescent or bioluminescent compound with anappropriate activation energy, either outside the subject or inside thesubject, with the chemiluminescence, phosphorescence or bioluminescencebeing allowed to activate the activatable pharmaceutical agent in vivoafter administration. The administration of the activatablepharmaceutical agent and the source of chemical energy can be performedsequentially in any order or can be performed simultaneously. In thecase of certain sources of such chemical energy, the administration ofthe chemical energy source can be performed after activation outside thesubject, with the lifetime of the emission of the energy being up toseveral hours for certain types of phosphorescent materials for example.There are no known previous efforts to use resonance energy transfer ofany kind to activate an intercalator to bind DNA.

In the PEPST embodiment of the present invention, the present inventionis significantly different from the phototherapy technique oftenreferred to as Photothermal Therapy (PTT). To illustrate the differencebetween the present invention PEPST, a form of photospectral therapy(PST) and the PTT technique, the photochemical processes involved in PSTand PPT is discussed below.

When drug molecules absorb excitation light, electrons undergotransitions from the ground state to an excited electronic state. Theelectronic excitation energy subsequently relaxes via radiative emission(luminescence) and radiation-less decay channels. When a moleculeabsorbs excitation energy, it is elevated from S₀ to some vibrationallevel of one of the excited singlet states, S_(n), in the manifold S₁, .. . , S_(n). In condensed media (tissue), the molecules in the S_(n)state deactivate rapidly, within 10⁻¹³ to 10⁻¹¹ s via vibrationalrelaxation (VR) processes, ensuring that they are in the lowestvibrational levels of S_(n) possible. Since the VR process is fasterthan electronic transitions, any excess vibrational energy is rapidlylost as the molecules are deactivated to lower vibronic levels of thecorresponding excited electronic state. This excess VR energy isreleased as thermal energy to the surrounding medium. From the S_(n)state, the molecule deactivates rapidly to the isoenergetic vibrationallevel of a lower electronic state such as S_(n-1) via an internalconversion (IC) process. IC processes are transitions between states ofthe same multiplicity. The molecule subsequently deactivates to thelowest vibronic levels of S_(n-1) via aVR process. By a succession of ICprocesses immediately followed by VR processes, the molecule deactivatesrapidly to the ground state S₁. This process results in excess VR and ICenergy released as thermal energy to the surrounding medium leading tothe overheating of the local environment surrounding the light absorbingdrug molecules. The heat produced results in local cell or tissuedestruction. The light absorbing species include natural chromophores intissue or exogenous dye compounds such as indocyanine green,naphthalocyanines, and porphyrins coordinated with transition metals andmetallic nanoparticles and nanoshells of metals. Natural chromophores,however, suffer from very low absorption. The choice of the exogenousphotothermal agents is made on the basis of their strong absorptioncross sections and highly efficient light-to-heat conversion. Thisfeature greatly minimizes the amount of laser energy needed to inducelocal damage of the diseased cells, making the therapy method lessinvasive. A problem associated with the use of dye molecules is theirphotobleaching under laser irradiation. Therefore, nanoparticles such asgold nanoparticles and nanoshells have recently been used. The promisingrole of nanoshells in photothermal therapy of tumors has beendemonstrated [Hirsch, L. R., Stafford, R. J., Bankson, J. A., Sershen,S. R., Rivera, B., Price, R. E., Hazle, J. D., Halas, N. J., and West,J. L., Nanoshell-mediated near-infrared thermal therapy of tumors undermagnetic resonance guidance. PNAS, 2003. 100(23): p. 13549-13554].

The PST method of the invention, however, is based on the radiativeprocesses (fluorescence, phosphorescence, luminescence, Raman, etc)whereas the PTT method is based on the radiationless processes (IC, VRand heat conversion) in molecules.

Various Light-Activated Pharmaceuticals

It has been reported that ferritin could be internalized by some tumortissues, and the internalization was associated with themembrane-specific receptors [S. Fargion, P. Arosio, A. L. Fracanzoni, V.Cislaghi, S. Levi, A. Cozzi, A Piperno and A. G. Firelli, Blood, 1988,71, 753-757; P. C. Adams, L. W. Powell and J. W. Halliday, Hepatology,1988, 8, 719-721]. Previous studies have shown that ferritin-bindingsites and the endocytosis of ferritin have been identified in neoplasticcells [M. S. Bretscher and J. N. Thomson, EMBO J., 1983, 2, 599-603].Ferritin receptors have the potential for use in the delivery ofanticancer drugs into the brain [S. W. Hulet, S. Powers and J. R.Connor, J. Neurol. Sci., 1999, 165, 48-55]. In one embodiment, theinvention uses ferritin or apoferritin to both encapsulate PA and energymodulation agent-PA systems and also target tumor cells selectively forenhanced drug delivery and subsequent phototherapy. In this case, noadditional bioreactors are needed.

The photoactive drug molecules can be given to a patient by oralingestion, skin application, or by intravenous injection. Thephotoactive drug molecules drugs travel through the blood stream insidethe body towards the targeted tumor (either via passive or activetargeting strategies). The invention treatment may also be used forinducing an auto vaccine effect for malignant cells, including those insolid tumors. To the extent that any rapidly dividing cells or stemcells may be damaged by a systemic treatment, then it may be preferableto direct the stimulating if, microwave, or magnetic induction energydirectly toward the tumor, preventing damage to most normal, healthycells or stem cells by avoiding photoactivation or resonant energytransfer of the photoactivatable agent.

Alternatively, a treatment may be applied that slows or pauses mitosis.Such a treatment is capable of slowing the division of rapidly dividinghealthy cells or stem cells during the treatment, without pausingmitosis of cancerous cells. Alternatively, a blocking agent isadministered preferentially to malignant cells prior to administeringthe treatment that slows mitosis.

In one embodiment, an aggressive cell proliferation disorder has a muchhigher rate of mitosis, which leads to selective destruction of adisproportionate share of the malignant cells during even a systemicallyadministered treatment. Stem cells and healthy cells may be spared fromwholesale programmed cell death, even if exposed to photoactivatedagents, provided that such photoactivated agents degenerate from theexcited state to a lower energy state prior to binding, mitosis or othermechanisms for creating damage to the cells of a substantial fraction ofthe healthy stem cells. Thus, an auto-immune response may not beinduced.

Alternatively, a blocking agent may be used that prevents or reducesdamage to stem cells or healthy cells, selectively, which wouldotherwise be impaired. The blocking agent is selected or is administeredsuch that the blocking agent does not impart a similar benefit tomalignant cells, for example.

In one embodiment, stem cells are targeted, specifically, fordestruction with the intention of replacing the stem cells with a donorcell line or previously stored, healthy cells of the patient. In thiscase, no blocking agent is used. Instead, a carrier or photosensitizeris used that specifically targets the stem cells.

Work in the area of photodynamic therapy has shown that the amount ofsinglet oxygen required to cause cell lysis, and thus cell death, is0.32×10⁻³ mol/liter or more, or 10⁹ singlet oxygen molecules/cell ormore. However, in one embodiment of the invention, it is most preferableto avoid production of an amount of singlet oxygen that would cause celllysis, due to its indiscriminate nature of attack, lysing both targetcells and healthy cells. Accordingly, it is most preferred in theinvention that the level of singlet oxygen production caused by theinitiation energy used or activatable pharmaceutical agent uponactivation be less than level needed to cause cell lysis.

In a further embodiment, methods in accordance with the invention mayfurther include adding an additive to alleviate treatment side-effects.Exemplary additives may include, but are not limited to, antioxidants,adjuvant, or combinations thereof. In one exemplary embodiment, psoralenis used as the activatable pharmaceutical agent, UV-A is used as theactivating energy, and antioxidants are added to reduce the unwantedside-effects of irradiation.

The activatable pharmaceutical agent and derivatives thereof as well asthe energy modulation agent and plasmonics compounds and structures, canbe incorporated into pharmaceutical compositions suitable foradministration. Such compositions typically comprise the activatablepharmaceutical agent and a pharmaceutically acceptable carrier. Thepharmaceutical composition also comprises at least one additive having acomplementary therapeutic or diagnostic effect, wherein the additive isone selected from an antioxidant, an adjuvant, or a combination thereof.

As used herein, “pharmaceutically acceptable carrier” is intended toinclude any and all solvents, dispersion media, coatings, antibacterialand antifungal agents, isotonic and absorption delaying agents, and thelike, compatible with pharmaceutical administration. The use of suchmedia and agents for pharmaceutically active substances is well known inthe art. Except insofar as any conventional media or agent isincompatible with the active compound, use thereof in the compositionsis contemplated. Supplementary active compounds can also be incorporatedinto the compositions. Modifications can be made to the compound of thepresent invention to affect solubility or clearance of the compound.These molecules may also be synthesized with D-amino acids to increaseresistance to enzymatic degradation. If necessary, the activatablepharmaceutical agent can be co-administered with a solubilizing agent,such as cyclodextran.

A pharmaceutical composition of the invention is formulated to becompatible with its intended route of administration. Examples of routesof administration include parenteral, e.g., intravenous, intradermal,subcutaneous, oral (e.g., inhalation), transdermal (topical),transmucosal, rectal administration, and direct injection into theaffected area, such as direct injection into a tumor. Solutions orsuspensions used for parenteral, intradermal, or subcutaneousapplication can include the following components: a sterile diluent suchas water for injection, saline solution, fixed oils, polyethyleneglycols, glycerin, propylene glycol or other synthetic solvents;antibacterial agents such as benzyl alcohol or methyl parabens;antioxidants such as ascorbic acid or sodium bisulfate; chelating agentssuch as ethylenediaminetetraacetic acid; buffers such as acetates,citrates or phosphates, and agents for the adjustment of tonicity suchas sodium chloride or dextrose. The pH can be adjusted with acids orbases, such as hydrochloric acid or sodium hydroxide. The parenteralpreparation can be enclosed in ampoules, disposable syringes or multipledose vials made of glass or plastic.

Pharmaceutical compositions suitable for injectable use include sterileaqueous solutions (where water soluble) or dispersions and sterilepowders for the extemporaneous preparation of sterile injectablesolutions or dispersion. For intravenous administration, suitablecarriers include physiological saline, bacteriostatic water, orphosphate buffered saline (PBS). In all cases, the composition must besterile and should be fluid to the extent that easy syringabilityexists. It must be stable under the conditions of manufacture andstorage and must be preserved against the contaminating action ofmicroorganisms such as bacteria and fungi. The carrier can be a solventor dispersion medium containing, for example, water, ethanol, polyol(for example, glycerol, propylene glycol, and liquid polyethyleneglycol, and the like), and suitable mixtures thereof. The properfluidity can be maintained, for example, by the use of a coating such aslecithin, by the maintenance of the required particle size in the caseof dispersion and by the use of surfactants. Prevention of the action ofmicroorganisms can be achieved by various antibacterial and antifungalagents, for example, parabens, chlorobutanol, phenol, ascorbic acid,thimerosal, and the like. In many cases, it will be preferable toinclude isotonic agents, for example, sugars, polyalcohols such asmanitol, sorbitol, sodium chloride in the composition. Prolongedabsorption of the injectable compositions can be brought about byincluding in the composition an agent which delays absorption, forexample, aluminum monostearate and gelatin.

Sterile injectable solutions can be prepared by incorporating the activecompound in the required amount in an appropriate solvent with one or acombination of ingredients enumerated above, as required, followed byfiltered sterilization. Generally, dispersions are prepared byincorporating the active compound into a sterile vehicle that contains abasic dispersion medium and the required other ingredients from thoseenumerated above. In the case of sterile powders for the preparation ofsterile injectable solutions, methods of preparation are vacuum dryingand freeze-drying that yields a powder of the active ingredient plus anyadditional desired ingredient from a previously sterile-filteredsolution thereof.

Oral compositions generally include an inert diluent or an ediblecarrier. They can be enclosed in gelatin capsules or compressed intotablets. For the purpose of oral therapeutic administration, the activecompound can be incorporated with excipients and used in the form oftablets, troches, or capsules. Oral compositions can also be preparedusing a fluid carrier for use as a mouthwash, wherein the compound inthe fluid carrier is applied orally and swished and expectorated orswallowed. Pharmaceutically compatible binding agents, and/or adjuvantmaterials can be included as part of the composition. The tablets,pills, capsules, troches and the like can contain any of the followingingredients, or compounds of a similar nature: a binder such asmicrocrystalline cellulose, gum tragacanth or gelatin; an excipient suchas starch or lactose, a disintegrating agent such as alginic acid,primogel, or corn starch; a lubricant such as magnesium stearate orSterotes; a glidant such as colloidal silicon dioxide; a sweeteningagent such as sucrose or saccharin; or a flavoring agent such aspeppermint, methyl salicylate, or orange flavoring.

For administration by inhalation, the compounds are delivered in theform of an aerosol spray from pressured container or dispenser whichcontains a suitable propellant, e.g., a gas such as carbon dioxide, or anebulizer.

Systemic administration can also be by transmucosal or transdermalmeans. For transmucosal or transdermal administration, penetrantsappropriate to the barrier to be permeated are used in the formulation.Such penetrants are generally known in the art, and include, forexample, for transmucosal administration, detergents, bile salts, andfusidic acid derivatives. Transmucosal administration can beaccomplished through the use of nasal sprays or suppositories. Fortransdermal administration, the active compounds are formulated intoointments, salves, gels, or creams as generally known in the art.

The compounds can also be prepared in the form of suppositories (e.g.,with conventional suppository bases such as cocoa butter and otherglycerides) or retention enemas for rectal delivery.

In one embodiment, the active compounds are prepared with carriers thatwill protect the compound against rapid elimination from the body, suchas a controlled release formulation, including implants andmicroencapsulated delivery systems. Biodegradable, biocompatiblepolymers can be used, such as ethylene vinyl acetate, polyanhydrides,polyglycolic acid, collagen, polyorthoesters, and polylactic acid.Methods for preparation of such formulations will be apparent to thoseskilled in the art. The materials can also be obtained commercially.Liposomal suspensions (including liposomes targeted to infected cellswith monoclonal antibodies to viral antigens) can also be used aspharmaceutically acceptable carriers. These can be prepared according tomethods known to those skilled in the art, for example, as described inU.S. Pat. No. 4,522,811, the entire contents of which are incorporatedherein by reference.

It is especially advantageous to formulate oral or parenteralcompositions in dosage unit form for ease of administration anduniformity of dosage. Dosage unit form as used herein refers tophysically discrete units suited as unitary dosages for the subject tobe treated; each unit containing a predetermined quantity of activecompound calculated to produce the desired therapeutic effect inassociation with the required pharmaceutical carrier. The specificationfor the dosage unit forms of the invention are dictated by and directlydependent on the unique characteristics of the active compound and theparticular therapeutic effect to be achieved, and the limitationsinherent in the art of compounding such an active compound for thetreatment of individuals.

The pharmaceutical compositions can be included in a container, pack,kit or dispenser together with instructions for administration.

Methods of administering agents are not limited to the conventionalmeans such as injection or oral infusion, but include more advanced andcomplex forms of energy transfer. For example, genetically engineeredcells that carry and express energy modulation agents may be used. Cellsfrom the host may be transfected with genetically engineered vectorsthat express bioluminescent agents. Transfection may be accomplished viain situ gene therapy techniques such as injection of viral vectors orgene guns, or may be performed ex vivo by removing a sample of thehost's cells and then returning to the host upon successfultransfection. Such transfected cells may be inserted or otherwisetargeted at the site where diseased cells are located.

It will also be understood that the order of administering the differentagents is not particularly limited. It will be appreciated thatdifferent combinations of ordering may be advantageously employeddepending on factors such as the absorption rate of the agents, thelocalization and molecular trafficking properties of the agents, andother pharmacokinetics or pharmacodynamics considerations.

An advantage of the methods of this approach is that by specificallytargeting cells affected by a cell proliferation disorder, such asrapidly dividing cells, and triggering a cellular change, such asapoptosis, in these cells in situ, the immune system of the host may bestimulated to have an immune response against the diseased cells. Oncethe host's own immune system is stimulated to have such a response,other diseased cells that are not treated by the activatablepharmaceutical agent may be recognized and be destroyed by the host'sown immune system. Such autovaccine effects may be obtained, forexample, in treatments using psoralen and UV-A.

The methods described here can be used alone or in combination withother therapies for treatment of cell proliferation disorders.Additionally, the methods described can be used, if desired, inconjunction with recent advances in chronomedicine, such as thatdetailed in Giacchetti et al, Journal of Clinical Oncology, Vol 24, No22 (August 1), 2006: pp. 3562-3569, the entire contents of which areincorporated herein by reference.

In chronomedicine, it has been found that cells suffering from certaintypes of disorders, such as cancer, respond better at certain times ofthe day than at others. Thus, chronomedicine could be used inconjunction with the present methods in order to augment the effect ofthe treatments of the invention.

Photobiomodulation

Another object of the invention is to treat a condition, disorder ordisease in a subject using an activatable pharmaceutical agent.Exemplary conditions, disorders or diseases may include, but are notlimited to, cancer, autoimmune diseases, cardiac ablasion (e.g., cardiacarrhythmia and atrial fibrillation), photoangioplastic conditions (e.g.,de novo atherosclerosis, restinosis), intimal hyperplasia, arteriovenousfistula, macular degeneration, psoriasis, acne, hopecia areata, portwinespots, hair removal, rheumatoid and inflammatory arthrisis, jointconditions, lymph node conditions, and cognitive and behavioralconditions.

Accordingly, the invention in one embodiment provides methods utilizingthe principle of energy transfer to and among molecular agents tocontrol delivery and activation of pharmaceutically active agents suchthat delivery of the desired pharmacological effect is more focused,precise, and effective than the conventional techniques. Here, theenergy transfer can include light from the gas containing up converterstructures of the invention.

Although not intending to be bound by any particular theory or beotherwise limited in any way, the following theoretical discussion ofscientific principles and definitions are provided to help the readergain an understanding and appreciation of the present invention.

As used here, the term “subject” is not intended to be limited tohumans, but may also include animals, plants, or any suitable biologicalorganism.

As used herein, the phrase “a disease or condition” refers to acondition, disorder or disease that may include, but are not limited to,cancer, soft and bone tissue injury, chronic pain, wound healing, nerveregeneration, viral and bacterial infections, fat deposits(liposuction), varicose veins, enlarged prostate, retinal injuries andother ocular diseases, Parkinson's disease, and behavioral, perceptionaland cognitive disorders. Exemplary conditions also may include nerve(brain) imaging and stimulation, a direct control of brain cell activitywith light, control of cell death (apoptosis), and alteration of cellgrowth and division. Yet other exemplary a condition, disorder ordisease may include, but are not limited to, cardiac ablasion (e.g.,cardiac arrhythmia and atrial fibrillation), photoangioplasticconditions (e.g., de novo atherosclerosis, restinosis), intimalhyperplasia, arteriovenous fistula, macular degeneration, psoriasis,acne, hopecia areata, portwine spots, hair removal, rheumatoid andinflammatory arthritis, joint conditions, and lymph node conditions.

As used here, the term “target structure” refers to an eukaryotic cell,prokaryotic cell, a subcellular structure, such as a cell membrane, anuclear membrane, cell nucleus, nucleic acid, mitochondria, ribosome, orother cellular organelle or component, an extracellular structure, virusor prion, and combinations thereof.

The nature of the predetermined cellular change will depend on thedesired pharmaceutical outcome. Exemplary cellular changes may include,but are not limited to, apoptosis, necrosis, up-regulation of certaingenes, down-regulation of certain genes, secretion of cytokines,alteration of cytokine receptor responses, regulation of cytochrome coxidase and flavoproteins, activation of mitochondria, stimulationantioxidant protective pathway, modulation of cell growth and division,alteration of firing pattern of nerves, alteration of redox properties,generation of reactive oxygen species, modulation of the activity,quantity, or number of intracellular components in a cell, modulation ofthe activity, quantity, or number of extracellular components producedby, excreted by, or associated with a cell, or a combination thereof.Predetermined cellular changes may or may not result in destruction orinactivation of the target structure.

As used here, an “energy modulation agent” refers to an agent that iscapable of receiving an energy input from a source and then re-emittinga different energy to a receiving target. The energy modulation agentscan be used in conjunction with gas containing up converter structuresof the invention to assist in the transfer of energy from the lightemitted from the gas containing up converter structures to thepharmaceutical agent or the photoactivatable agent or to the tissuebeing treated.

Energy transfer among molecules may occur in a number of ways. The formof energy may be electronic, thermal, electromagnetic, kinetic, orchemical in nature. Energy may be transferred from one molecule toanother (intermolecular transfer) or from one part of a molecule toanother part of the same molecule (intramolecular transfer). Forexample, a modulation agent may receive electromagnetic energy andre-emit the energy in the form of thermal energy. In variousembodiments, the energy modulation agents (e.g., the gas containing upconverter structures) receive RF or microwave energy and re-emits athigher energy (e.g. UV-A, UV-B, visible). In various embodiments, theenergy modulation agents receive higher energy (e.g. x-ray) and re-emitsin lower energy (e.g. UV-A). Some modulation agents may have a veryshort energy retention time (on the order of fs, e.g. fluorescentmolecules) whereas others may have a very long half-life (on the orderof minutes to hours, e.g. luminescent or phosphorescent molecules).Suitable energy modulation agents include, but are not limited to, abiocompatible fluorescing metal nanoparticle, fluorescing dye molecule,gold nanoparticle, a water soluble quantum dot encapsulated bypolyamidoamine dendrimers, a luciferase, a biocompatible phosphorescentmolecule, a combined electromagnetic energy harvester molecule, and alanthanide chelate capable of intense luminescence. Various exemplaryuses of these are described below in preferred embodiments.

The modulation agents may further be coupled to a carrier for cellulartargeting purposes. For example, a biocompatible molecule, such as afluorescing metal nanoparticle or fluorescing dye molecule that emits inthe UV-A band, may be selected as the energy modulation agent.

The energy modulation agent may be preferably directed to the desiredsite (e.g. a tumor) by systemic administration to a subject. Forexample, a UV-A emitting energy modulation agent may be concentrated inthe tumor site by physical insertion or by conjugating the UV-A emittingenergy modulation agent with a tumor specific carrier, such as a lipid,chitin or chitin-derivative, a chelate or other functionalized carrierthat is capable of concentrating the UV-A emitting source in a specifictarget tumor.

Additionally, the energy modulation agent can be used alone or as aseries of two or more other energy modulation agents wherein the energymodulation agents provide an energy cascade. Thus, the first energymodulation agent in the cascade will absorb the activation energy,convert it to a different energy which is then absorbed by the secondenergy modulation in the cascade, and so forth until the end of thecascade is reached with the final energy modulation agent in the cascadeemitting the energy necessary to activate the activatable pharmaceuticalagent.

Signals that may be used to activate a corresponding agent may include,but are not limited to, photons of specific wavelengths (e.g. x-rays,ultraviolet, or visible light), electromagnetic energy (e.g. radio ormicrowave), thermal energy, acoustic energy, or any combination thereof.

Activation of the agent may be as simple as delivering the signal to theagent or may further premise on a set of activation conditions. Forexample, an activatable pharmaceutical agent, such as a photosensitizer,may be activated by UV-A radiation from the gas containing up converterstructures of the invention. Once activated, the agent in itsactive-state may then directly proceed to effect a cellular change.

Where activation may further premise upon other conditions, meredelivery of the activation signal may not be sufficient to bring aboutthe desired cellular change. For example, a photoactive compound thatachieves its pharmaceutical effect by binding to certain cellularstructure in its active state may require physical proximity to thetarget cellular structure when the activation signal is delivered. Forsuch activatable agents, delivery of the activation signal undernon-activating conditions will not result in the desired pharmacologiceffect. Some examples of activating conditions may include, but are notlimited to, temperature, pH, location, state of the cell, presence orabsence of co-factors.

Selection of an activatable pharmaceutical agent greatly depends on anumber of factors such as the desired cellular change, the desired formof activation, as well as the physical and biochemical constraints thatmay apply. Exemplary activatable pharmaceutical agents may include, butare not limited to, agents that may be activated by photonic energy,electromagnetic energy, acoustic energy, chemical or enzymaticreactions, thermal energy, or any other suitable activation mechanisms.

When activated, the activatable pharmaceutical agent may effect cellularchanges that include, but are not limited to, apoptosis, redirection ofmetabolic pathways, up-regulation of certain genes, down-regulation ofcertain genes, secretion of cytokines, alteration of cytokine receptorresponses, or combinations thereof.

The mechanisms by which an activatable pharmaceutical agent may achieveits desired effect are not particularly limited. Such mechanisms mayinclude direct action on a predetermined target as well as indirectactions via alterations to the biochemical pathways. A preferred directaction mechanism is by binding the agent to a critical cellularstructure such as nuclear DNA, mRNA, rRNA, ribosome, mitochondrial DNA,or any other functionally important structures. Indirect mechanisms mayinclude releasing metabolites upon activation to interfere with normalmetabolic pathways, releasing chemical signals (e.g. agonists orantagonists) upon activation to alter the targeted cellular response,and other suitable biochemical or metabolic alterations.

In one embodiment, the activatable pharmaceutical agent is capable ofchemically binding to the DNA or mitochondria at therapeuticallyeffective amount. In this embodiment, the activatable pharmaceuticalagent, preferably a photoactivatable agent, is exposed in situ to anactivating energy emitted from an energy modulation agent, which, inturn receives energy from an initiation energy source. An activatableagent may be a small molecule; a biological molecule such as a protein,a nucleic acid or lipid; a supramolecular assembly; a nanoparticle; orany other molecular entity having a pharmaceutical activity onceactivated.

The activatable agent may be derived from a natural or synthetic origin.Any such molecular entity that may be activated by a suitable activationsignal source to effect a predetermined cellular change may beadvantageously employed in the present invention.

Suitable photoactive agents include, but are not limited to: psoralensand psoralen derivatives, pyrene cholesteryloleate, acridine, porphyrin,fluorescein, rhodamine, 16-diazorcortisone, ethidium, transition metalcomplexes of bleomycin, transition metal complexes of deglycobleomycin,organoplatinum complexes, alloxazines such as 7,8-dimethyl-10-ribitylisoalloxazine (riboflavin), 7,8,10-trimethylisoalloxazine (lumiflavin),7,8-dimethylalloxazine (lumichrome), isoalloxazine-adenine dinucleotide(flavine adenine dinucleotide [FAD]), alloxazine mononucleotide (alsoknown as flavine mononucleotide [FMN] and riboflavine-5-phosphate),vitamin Ks, vitamin L, their metabolites and precursors, andnapththoquinones, naphthalenes, naphthols and their derivatives havingplanar molecular conformations, porphyrins, dyes such as neutral red,methylene blue, acridine, toluidines, flavine (acriflavinehydrochloride) and phenothiazine derivatives, coumarins, quinolones,quinones, and anthroquinones, aluminum (111) phthalocyaninetetrasulfonate, hematoporphyrin, and phthalocyanine, and compounds whichpreferentially adsorb to nucleic acids with little or no effect onproteins. The term “alloxazine” includes isoalloxazines.

Endogenously-based derivatives include synthetically derived analogs andhomologs of endogenous photoactivated molecules, which may have or lacklower (1 to 5 carbons) alkyl or halogen substituents of thephotosensitizers from which they are derived, and which preserve thefunction and substantial non-toxicity. Endogenous molecules areinherently non-toxic and may not yield toxic photoproducts afterphotoradiation.

The initiation energy source can be any energy source capable ofproviding energy at a level sufficient to cause cellular changesdirectly or via a modulation agent which transfer the initiation energyto energy capable of causing the predetermined cellular changes. Also,the initiation energy source can be any energy source capable ofproviding energy at a level sufficient activate the activatable agentdirectly, or to provide the energy to a modulation agent with the inputneeded to emit the activation energy for the activatable agent (indirectactivation). In one embodiment, the initiation energy is capable ofpenetrating completely through the subject. Within the context of theinvention, the phrase “capable of penetrating completely through thesubject” is used to refer to energy that can penetrate to any depthwithin the subject to activate the activatable pharmaceutical agent. Itis not required that the any of the energy applied actually passcompletely through the subject, merely that it be capable of doing so inorder to permit penetration to any desired depth to activate theactivatable pharmaceutical agent. Exemplary initiation energy sourcesthat are capable of penetrating completely through the subject include,but are not limited to, UV light, visible light, IR radiation, x-rays,gamma rays, electron beams, microwaves and radio waves.

An additional embodiment of the invention is to provide a method fortreatment of a condition, disease or disorder by the in-situ generationof energy in a subject in need thereof, where the energy generated canbe used directly to effect a change thereby treating the condition,disease or disorder, or the energy can be used to activate anactivatable pharmaceutical agent, which upon activation effects a changethereby treating the condition, disease or disorder. The energy can begenerated in-situ by any desired method, including, but not limited to,chemical reaction such as chemiluminescence, or by conversion of anenergy applied to the subject externally, which is converted in-situ toa different energy (of lower or higher energy than that applied),through the use of one or more energy modulation agents.

A further embodiment of the invention combines the treatment of acondition, disease or disorder with the generation of heat in theaffected target structure in order to enhance the effect of thetreatment. For example, in the treatment of a cell proliferationdisorder using a photoactivatable pharmaceutical agent (such as apsoralen or derivative thereof), one can activate the photoactivatablepharmaceutical agent by applying an initiation energy which, directly orindirectly, activates the pharmaceutical agent. As noted elsewhere inthis application, this initiation energy can be of any type, so long asit can be converted to an energy suitable for activating thepharmaceutical compound. In addition to applying this initiation energy,in this embodiment of the present invention, an energy is applied thatcauses heating of the target structure. In the case of a cellproliferation disorder such as cancer, the heating would increase theproliferation rate of the cancer cells. While this may seemcounterintuitive at first, when the cell proliferation disorder is beingtreated using a DNA intercalation agent, such as psoralen or aderivative thereof, this increase in cell proliferation can actuallyassist the psoralen in causing apoptosis. In particular, when psoralenbecomes intercalated into DNA, apoptosis occurs when the cell goesthrough its next division cycle. By increasing the rate at which thecells divide, one can use the present invention methods to enhance theonset of apoptosis.

In one embodiment, heat can be generated by any desired manner.Preferably, the heat can be generated using the application ofmicrowaves or NIR energy to the target structure or by the use of use ofnanoparticles of metal or having metal shells. Heat can also begenerated by the absorption of light from the gas containing upconverter structures of the invention. Alternatively, as is done intumor thermotherapy, magnetic metal nanoparticles can be targeted tocancer cells using conventional techniques, then used to generate heatby application of a magnetic field to the subject under controlledconditions. (DeNardo S J, DeNardo G L, Natarajan A et al.: Thermaldosimetry predictive of efficacy of 111In-ChL6 NPAMF-inducedthermoablative therapy for human breast cancer in mice. J. Nucl.Med.48(3), 437-444 (2007).)

In another embodiment, the patient's own cells are removed andgenetically modified to provide photonic emissions. For example, tumoror healthy cells may be removed, genetically modified to inducebioluminescence and may be reinserted at the site of the disease orcondition to be treated. The modified, bioluminescent cells may befurther modified to prevent further division of the cells or division ofthe cells only so long as a regulating agent is present.

In a further embodiment, a biocompatible emitting source, such as afluorescing metal nanoparticle or fluorescing dye molecule or the gascontaining up converter structures of the invention, is selected thatemits in the UV-A band. The UV-A emitting source is directed to the siteof a disease or condition. The UV-A emitting source may be directed tothe site of the disease or condition by systemically administering theUV-A emitting source. Preferably, the UV-A emitting source isconcentrated in the target site, such as by physical insertion or byconjugating the UV-A emitting molecule with a specific carrier that iscapable of concentrating the UV-A emitting source in a specific targetstructure, as is known in the art.

In another embodiment, a UV- or light-emitting luciferase is selected asthe emitting source for exciting a photoactivatable agent. A luciferasemay be combined with ATP or another molecule, which may then beoxygenated with additional molecules to stimulate light emission at adesired wavelength. Alternatively, a phosphorescent emitting source maybe used. One advantage of a phosphorescent emitting source is that thephosphorescent emitting molecules or other source may beelectroactivated or photoactivated prior to insertion into a target siteeither by systemic administration or direct insertion into the region ofthe target site. Alternatively, some of these materials can beactivated, with the energy being “stored” in the activated material,until emission is stimulated by application of another energy. Forexample, see the discussion in U.S. Pat. No. 4,705,952 (incorporated byreference in its entirety) regarding infrared-triggered phosphors.

Phosphorescent materials may have longer relaxation times thanfluorescent materials, because relaxation of a triplet state is subjectto forbidden energy state transitions, storing the energy in the excitedtriplet state with only a limited number of quantum mechanical energytransfer processes available for returning to the lower energy state.Energy emission is delayed or prolonged from a fraction of a second toseveral hours. Otherwise, the energy emitted during phosphorescentrelaxation is not otherwise different than fluorescence, and the rangeof wavelengths may be selected by choosing a particular phosphor.

Among various materials, luminescent nanoparticles have attractedincreasing technological and industrial interest. In the context of theinvention, nanoparticle refers to a particle having a size less than onemicron. While the description of the invention describes specificexamples using nanoparticles, the invention in many embodiments is notlimited to particles having a size less than one micron. However, inmany of the embodiments, the size range of having a size less than onemicron, and especially less than 100 nm produces properties of specialinterest such as for example emission lifetime luminescence quenching,luminescent quantum efficiency, and concentration quenching and such asfor example diffusion, penetration, and dispersion into mediums wherelarger size particles would not migrate.

In an additional embodiment, the photoactivatable agent can be aphotocaged complex having an active agent contained within a photocage.The active agent is bulked up with other molecules that prevent it frombinding to specific targets, thus masking its activity. When thephotocage complex is photoactivated, the bulk falls off, exposing theactive agent. In such a photocage complex, the photocage molecules canbe photoactive (i.e. when photoactivated, they are caused to dissociatefrom the photocage complex, thus exposing the active agent within), orthe active agent can be the photoactivatable agent (which whenphotoactivated causes the photocage to fall off), or both the photocageand the active agent are photoactivated, with the same or differentwavelengths. For example, a toxic chemotherapeutic agent can bephotocaged, which will reduce the systemic toxicity when delivered. Oncethe agent is concentrated in the tumor, the agent is irradiated with anactivation energy. This causes the “cage” to fall off, leaving acytotoxic agent in the tumor cell. Suitable photocages include thosedisclosed by Young and Deiters in “Photochemical Control of BiologicalProcesses”, Org. Biomol. Chem., 5, pp. 999-1005 (2007) and“Photochemical Hammerhead Ribozyme Activation”, Bioorganic & MedicinalChemistry Letters, 16(10), pp. 2658-2661 (2006), the contents of whichare hereby incorporated by reference.

In one embodiment, the use of light (e.g. light emitted from the gascontaining up converter structures) for uncaging a compound or agent isused for elucidation of neuron functions and imaging, for example,two-photon glutamine uncaging (Harvey C D, et al., Nature, 450:1195-1202(2007); Eder M, et al., Rev. Neurosci., 15:167-183 (2004)). Othersignaling molecules can be released by UV light stimulation, e.g., GABA,secondary messengers (e.g., Ca²⁺ and Mg²⁺), carbachol, capsaicin, andATP (Zhang F., et al., 2006). Chemical modifications of ion channels andreceptors may be carried out to render them light-responsive. Ca²⁺ isinvolved in controlling fertilization, differentiation, proliferation,apoptosis, synaptic plasticity, memory, and developing axons. In yetanother preferred embodiment, Ca²⁺ waves can be induced by UVirradiation (single-photon absorption) and NIR irradiation (two-photonabsorption) by releasing caged Ca²⁺, an extracellular purinergicmessenger InsP3 (Braet K., et al., Cell Calcium, 33:37-48 (2003)), orion channel ligands (Zhang F., et al., 2006).

Genetic targeting allows morphologically and electrophysipologicallycharacterization of genetically defined cell populations. Accordingly,in an additional embodiment, a light-sensitive protein is introducedinto cells or live subjects via a number of techniques includingelectroporation, DNA microinjection, viral delivery, liposomaltransfection, creation of transgenic lines and calcium-phosphateprecipitation. For example, lentiviral technology provides a convenientcombination a conventional combination of stable long-term expression,ease of high-titer vector production and low immunogenicity. Thelight-sensitive protein may be, for example, channelrhodopsin-2 (ChR2)and chloride pump halorhodopsin (NpHR). The light protein encodinggene(s) along with a cell-specific promoter can be incorporated into thelentiviral vector or other vector providing delivery of thelight-sensitive protein encoding gene into a target cell. ChR2containing a light sensor and a cation channel, provides electricalstimulation of appropriate speed and magnitude to activate neuronalspike firing, when the cells harboring Ch2R are pulsed with light.

In one embodiment, a lanthanide chelate capable of intense luminescencecan be used. For example, a lanthanide chelator may be covalently joinedto a coumarin or coumarin derivative or a quinolone orquinolone-derivative sensitizer. Sensitizers may be a 2- or 4-quinolone,a 2- or 4-coumarin, or derivatives or combinations of these examples. Acarbostyril 124 (7-amino-4-methyl-2-quinolone), a coumarin 120(7-amino-4-methyl-2-coumarin), a coumarin 124(7-amino-4-(trifluoromethyl)-2-coumarin), aminoinethyltrimethylpsoralenor other similar sensitizer may be used. Chelates may be selected toform high affinity complexes with lanthanides, such as terbium oreuropium, through chelator groups, such as DTPA. Such chelates may becoupled to any of a wide variety of well known probes or carriers, andmay be used for resonance energy transfer to a psoralen orpsoralen-derivative, such as 8-MOP, or other photoactive moleculescapable of binding DNA. In one alternative example, the lanthanidechelate is localized at the site of the disease using an appropriatecarrier molecule, particle or polymer, and a source of electromagneticenergy is introduced by minimally invasive procedures (e.g., the gascontaining upconverters of the invention) to irradiate the targetstructure, after exposure to the lanthanide chelate and a photoactivemolecule.

In another embodiment, a biocompatible, endogenous fluorophore emittercan be selected to stimulate resonance energy transfer to aphotoactivatable molecule. A biocompatible emitter (e.g. the gascontaining up converter structures) with an emission maxima within theabsorption range of the biocompatible, endogenous fluorophore emittermay be selected to stimulate an excited state in fluorophore emitter.One or more halogen atoms may be added to any cyclic ring structurecapable of intercalation between the stacked nucleotide bases in anucleic acid (either DNA or RNA) to confer new photoactive properties tothe intercalator. Any intercalating molecule (psoralens, coumarins, orother polycyclic ring structures) may be selectively modified byhalogenation or addition of non-hydrogen bonding ionic substituents toimpart advantages in its reaction photochemistry and its competitivebinding affinity for nucleic acids over cell membranes or chargedproteins, as is known in the art.

Skin photosensitivity is a major toxicity of photosensitizers. Severesunburn occurs if skin is exposed to direct sunlight for even a fewminutes. Early murine research hinted at a vigorous and long termstimulation of immune response; however, actual clinical testing hasfailed to achieve the early promises of photodynamic therapies. Theearly photosensitizers for photodynamic therapies targeted type IIresponses, which created singlet oxygen when photoactivated in thepresence of oxygen. The singlet oxygen caused cellular necrosis and wasassociated with inflammation and an immune response. Some additionalphotosensitizers have been developed to induce type I responses,directly damaging cellular structures.

Porfimer sodium (Photofrin; QLT Therapeutics, Vancouver, BC, Canada), isa partially purified preparation of hematoporphyrin derivative (HpD).Photofrin has been approved by the US Food and Drug Administration forthe treatment of obstructing esophageal cancer, microinvasiveendobronchial non-small cell lung cancer, and obstructing endobronchialnon-small cell lung cancer. Photofrin is activated with 630 nm, whichhas a tissue penetration of approximately 2 to 5 mm. Photofrin has arelatively long duration of skin photosensitivity (approximately 4 to 6weeks).

Tetra (m-hydroxyphenyl) chlorin (Foscan; Scotia Pharmaceuticals,Stirling, UK), is a synthetic chlorine compound that is activated by 652nm light. Clinical studies have demonstrated a tissue effect of up to 10mm with Foscan and 652 nm light. Foscan is more selectively aphotosensitizer in tumors than normal tissues, and requires acomparatively short light activation time. A recommended dose of 0.1mg/kg is comparatively low and comparatively low doses of light may beused. Nevertheless, duration of skin photosensitivity is reasonable(approximately 2 weeks). However, Foscan induces a comparatively highyield of singlet oxygen, which may be the primary mechanism of DNAdamage for this molecule.

Motexafin lutetium (Lutetium texaphryin) is activated by light in thenear infared region (732 nm). Absorption at this wavelength has theadvantage of potentially deeper penetration into tissues, compared withthe amount of light used to activate other photosensitizers (FIGS. 2Aand 2B). Lutetium texaphryin also has one of the greatest reportedselectivities for tumors compared to selectivities of normal tissues.Young S W, et al.: Lutetium texaphyrin (PCI-0123) a near-infrared,water-soluble photosensitizer. Photochem Photobiol 1996, 63:892-897. Inaddition, its clinical use is associated with a shorter duration of skinphotosensitivity (24 to 48 hours). Lutetium texaphryin has beenevaluated for metastatic skin cancers. It is currently underinvestigation for treatment of recurrent breast cancer and for locallyrecurrent prostate cancer. The high selectivity for tumors promisesimproved results in clinical trials.

In general, the approach may be used with any source for the excitationan activatable molecule. The process may be a photopheresis process ormay be similar to photophoresis. While photophoresis is generallythought to be limited to photonic excitation, such as by UV-light, otherforms of radiation may be used as a part of a system to activate anactivatable molecule. Light emission can stimulate the activation of anactivatable molecule, such as 8-MOP. In one example, light emission fromthe gas containing up converter structures of the invention is directedat a solid tumor and stimulates, directly or indirectly, activation of8-MOP.

In yet another embodiment, the activatable pharmaceutical agent,preferably a photoactive agent, is directed to a receptor site by acarrier having a strong affinity for the receptor site. The carrier maybe a polypeptide and may form a covalent bond with a photo active agent,for example. The polypeptide may be an insulin, interleukin,thymopoietin or transferrin, for example. Alternatively, a photoactivepharmaceutical agent may have a strong affinity for the target cellwithout a binding to a carrier.

For example, a treatment may be applied that acts to slow or pausemitosis. Such a treatment is capable of slowing the division of rapidlydividing healthy cells or stem cells without pausing mitosis ofcancerous cells. Thus, the difference in growth rate between thenon-target cells and target cells are further differentiated to enhancethe effectiveness of the methods of the invention.

In a further embodiment, methods in accordance with the invention mayfurther include adding an additive to alleviate treatment side-effects.Exemplary additives may include, but are not limited to, antioxidants,adjuvant, or combinations thereof. In one exemplary embodiment, psoralenis used as the activatable pharmaceutical agent, UV-A is used as theactivating energy, and antioxidants are added to reduce the unwantedside-effects of irradiation.

In another aspect, the invention also provides methods for producing anautovaccine, including: (1) providing a population of targeted cells;(2) treating the cells ex vivo with a psoralen or a derivative thereof(3) activating the psoralen with an initiation energy source to induce apredetermined change in a target structure in the population of thetarget cells; and (4) returning the treated cells back to the host toinduce an autovaccine effect against the targeted cell, wherein thetreated cells cause an autovaccine effect.

In another aspect, heat can be generated in the target structure fromthe light from the at least one gas containing up converter structure,and the heat can enhance the induction of the predetermined change. Inthis embodiment, the predetermined change can modify the targetstructure and modulate the biological activity of the target structurethus treating a condition, disorder or disease affecting the targetstructure.

In one example of modulating biological activity, microwave drivenplasma UV emission sources have been used to activate psoralen in testcultures containing B16 melanoma cancer cells or PC3 prostate tumorcells. FIG. 79A represents a schematic of the in-vitro assay depictingthe clonogenic survival assays used to test if the microwaves canactivate the drug TMP to kill cancer cells. Cells were exposed, througha phantom to mimic in-vivo penetration of the activation energy, to one,five or ten minutes of light generated via a microwave driven plasma UVemission. Compared to controls, significantly more cancer cells werekilled with the TMP activated by plasma generated UV light. For thelonger exposure times, 5 minutes and greater, some of the cell kill canlikely be attributed to hyperthermia effects. FIG. 79B shows that theMRI seems very efficient with UV-stratalinker bulbs at activating TMP inPC3 cells. Even as little as a 1 min exposure was sufficient to killalmost all the cells. The decrease in survival seen in the DMSO/vehiclegroups treated at 5 min and 10 min exposures is likely due tohyperthermic cell kill. The temperatures of the media post-10 minexposure ranged from 39-43° C., which is high enough to negativelyeffect survival.

Generalized Upconversion

The invention as described above can be viewed for its aspects ofexposing an up converter to one source of light or radiation (aninitiation source for exampled of a relatively low energy) and havingthe up converter produce light or radiation at a relatively higherenergy. In one embodiment of the invention, a change is produced in amedium. The change is produced by (1) placing in a vicinity of themedium the upconverter or an otherwise upconverting structure, and (2)applying the initiation energy from an energy source through theartificial container to the medium, wherein the emitted light directlyor indirectly produces the change in the medium. As explained above, forthe upconverter to be placed in a vicinity of the medium to be changed(i.e. the upconverter can be within the medium, partly inside or outsidethe medium, or segregated outside the medium). The resultant of theupconverter being placed in a vicinity of the medium is that emittedlight from the upconverter is incident on the medium, thereby directlyor indirectly producing the change in the medium.

The upconverter or the otherwise upconverting structure in oneembodiment is configured, upon exposure to a first wavelength λ₁ ofradiation, to generate a second wavelength λ₂ of radiation having ahigher energy than the first wavelength λ₁. The upconverter or theotherwise upconverting structure in one embodiment includes a metallicshell encapsulating at least a fraction of the nanoparticle.

The change produced can cure a radiation-curable medium by activating aphotoinitiator in the radiation-curable medium. In this case, theemitted light can be of a wavelength appropriate to inducephoto-catalytic effects such as coupling to a photoinitiator or a UVcross-linking agent to produce curing in the uncured medium. Curing orpolymerization of the medium results in the formation of a partial orcomplete three-dimensional network. The radiation-curable medium can becured by activating a photoinitiator in the radiation-curable medium.For way of contrast, an uncured state of a material can be considered astate at which the material exhibit liquid-like behavior with aviscosity that can be high or that can be low. The cured state typicallyresults in a state at which the material exhibits solid-like orrubbery-like behavior or a visco-elastic behavior and can result in astate where limited flow under an applied stress is produced.

The change produced can result in a photo-stimulated change to a medium.The change produced can result in a radiation cured medium. The changeproduced can result in a sterilized medium. The change produced canactivate therapeutic drug.

For many applications, the initiation source may well be low frequencysources such as microwave or radio frequency irradiation, where in oneembodiment of the invention localized heating of the agent enhancesgeneration of a secondary light and in another embodiment localizedfield enhancements from the microwave field present in the mediumenhance fluorescence, as described in “Microwave-AcceleratedMetal-Enhanced Fluorescence (Mamef) With Silver Colloids in 96-WellPlates: Application to Ultra Fast and Sensitive Immunoassays, HighThroughput Screening and Drug Discovery,” by Aslan et al in Journal ofImmunological Methods 312 (2006) 137-147.

For many applications, the initiation source is a low frequency sourcesuch as microwave or radiofrequency irradiation, where in one embodimentof the invention absorption of the microwave radiation by the gascontaining up converter structures results in subsequent emission athigher energies toward the infrared, visible, and ultraviolet. Thedegree to which the upconverted radiation is applicable to theapplications described above will be dependent on the conversionefficiencies and will be dependent on the efficiency of a recipientmolecule linked to the specific metal shell/dielectric corenanostructures to absorb the upconverted light. The recipient moleculemay linked to the upconverters to absorb the upconverted light.

For many applications, the initiation source may well be low frequencysources such as microwave or radio frequency irradiation, where in oneembodiment of the invention the low frequency sources and evenultrasound sources interact with a component in the up convertingstructure to produce light for example by plasma excitation of a gas inthe upconverting structure or activation of a chemical reaction in theupconverting structure.

In one embodiment, the invention utilizes microwave or radiofrequencyenergy to promote light generation from the upconverter or upconvertinggas structure, whose light emission in turn produces a number of thephysical and biological changes described above.

In one embodiment of the invention, the initiation energy source is atleast one of x-rays, high energy particles, microwaves, radio waves, ormagnetic induction. The x-rays and high energy particles may used assources for generating free electrons inside the gas containing upconverters of the invention. The generated free electrons ay then gainenergy through the applied microwaves, radio waves, or magneticinduction fields.

In one embodiment of the invention, at least one activatablepharmaceutical agent that is capable of activation a predeterminedcellular change when activated is administering to a subject. Light fromthe at least one upconverter interacts with the at least one activatablepharmaceutical agent to activate the activatable pharmaceutical agent insitu, thus causing the predetermined cellular change to occur in themedium of the subject.

In one embodiment of the invention, the initiation energy is capable ofpenetrating completely through the subject.

In one embodiment of the invention, the cell proliferation disorder isat least one member selected from the group consisting of cancer,bacterial infection, viral infection, immune rejection response,autoimmune disorders, aplastic conditions, and combinations thereof. Inone embodiment of the invention, the activatable pharmaceutical agent isa photoactivatable agent. The activatable pharmaceutical agent can beselected from psoralens, pyrene cholesteryloleate, acridine, porphyrin,fluorescein, rhodamine, 16-diazorcortisone, ethidium, transition metalcomplexes of bleomycin, transition metal complexes of deglycobleomycinorganoplatinum complexes, alloxazines, vitamin Ks, vitamin L, vitaminmetabolites, vitamin precursors, naphthoquinones, naphthalenes,naphthols and derivatives thereof having planar molecular conformations,porphorinporphyrins, dyes and phenothiazine derivatives, coumarins,quinolones, quinones, and anthroquinones.

In one embodiment of the invention, the pharmaceutical agent is apsoralen, a coumarin, a porphyrin or a derivative thereof. In oneembodiment of the invention, the pharmaceutical agent is 8-MOP or AMT.In one embodiment of the invention, the activatable pharmaceutical agentis one selected from 7,8-dimethyl-10-ribityl, isoalloxazine,7,8,10-trimethylisoalloxazine, 7,8-dimethylalloxazine,isoalloxazine-adenine dinucleotide, alloxazine mononucleotide, aluminum(III) phthalocyanine tetrasulonate, hematophorphyrin, andphthadocyanine.

In one embodiment of the invention, the activatable pharmaceutical agentis coupled to a carrier that is capable of binding to a receptor site.The carrier can be one selected from insulin, interleukin, thymopoietinor transferrin. In one embodiment of the invention, the activatablepharmaceutical agent is coupled to the carrier by a covalent bond. Inone embodiment of the invention, the activatable pharmaceutical agent iscoupled to the carrier by non-covalent bond. In one embodiment of theinvention, the receptor site is one selected from nucleic acids ofnucleated cells, antigenic sites on nucleated cells, or epitopes.

In one embodiment of the invention, the pharmaceutical agent hasaffinity for a target cell. In one embodiment of the invention, theactivatable pharmaceutical agent is capable of being preferentiallyabsorbed by a target cell. In one embodiment of the invention, thepredetermined cellular change is apoptosis in a target cell.

In one embodiment of the invention, the activatable pharmaceutical agentcauses an auto-vaccine effect in the subject that reacts with a targetcell. The auto-vaccine effect can be generated in a joint or lymph node.In one embodiment of the invention, the activatable pharmaceutical agentis a DNA intercalator or a halogenated derivative thereof.

In one embodiment of the invention, light from the at least oneupconverter is applied to a target structure in a subject in need oftreatment, wherein the light contacts the target structure and induces apredetermined change in the target structure in situ in the medium ofthe subject, and the predetermined change modifies the target structureand modulates the biological activity of the target structure. In thisembodiment, the initiation energy can be capable of penetratingcompletely through the subject. In this embodiment, the light can inducea predetermined change in the target structure with or without an energymodulator or photoactive agent.

In this embodiment, an energy modulation agent can be administered tothe subject which adsorbs, intensifies or modifies the light into anenergy that effects the predetermined change in the target structure. Inthis embodiment, the energy modulation agent can be specifically locatedaround, on, or in the target structure. In this embodiment, the energymodulation agent can also transform the initiation electromagneticenergy into a photonic or another electromagnetic energy that effectsthe predetermined change in the target structure. In this embodiment,the energy modulation agent can decrease the wavelength of theinitiation energy. In this embodiment, the energy modulation agent canincrease the wavelength of the initiation energy. In this embodiment,the energy modulation agent(s) can include one or more members selectedfrom a biocompatible fluorescing metal nanoparticle, fluorescing metaloxide nanoparticle, fluorescing metal coated metal oxide nanoparticle,fluorescing dye molecule, gold nanoparticle, silver nanoparticle,gold-coated silver nanoparticle, a water soluble quantum dotencapsulated by polyamidoamine dendrimers, a luciferase, a biocompatiblephosphorescent molecule, a combined electromagnetic energy harvestermolecule, and a lanthanide chelate exhibiting intense luminescence.

In this embodiment, the predetermined change can or can not result indestruction, lysis orinactivation of the target structure. In thisembodiment, the predetermined change can enhance an activity of thetarget structure. The activity enhanced can be energy emission from thetarget, which then mediates, initiates or enhances a biological activityof other target structures in the subject, or of a second targetstructure.

In this embodiment, the target structure can be at least one of aeukaryotic cell, a prokaryotic cell, a subcellular structure. Thesubcellular structure can be a cell membrane, a nuclear membrane, cellnucleus, nucleic acid, mitochondria, ribosome, or other cellularorganelle or component. In this embodiment, the target structure can beat least one of an extracellular structure, a virus or prion, a cellulartissue.

In this embodiment, the predetermined change can result in treatment ofa condition, disorder or disease in the subject. The condition, disorderor disease can be at least one of a cancer, a disease occurring in asoft tissue and/or cartilage, a disease occurring in bone tissue, achronic pain, an autoimmune disease, a prion, viral, bacterial, fungal,or parasitic infection, a disease characterized by varicose veins, adisease characterized by an enlarged prostate, a disease characterizedby retinal injuries and other ocular diseases, a disease characterizedby a behavioral, perceptional and/or cognitive disorder, or Parkinson'sdisease.

In this embodiment, the predetermined change can be a wound healing, anenhancement of tissue growth, nerve regeneration or sensoryregeneration/restoration, reduction or removal of fat deposits(liposuction), nerve (brain) imaging and stimulation or direct controlof brain cell activity with light, modulation of cell death (apoptosis),modulating cell growth and division, modulation of an activity,quantity, or number of intracellular components in a cell, ormodulationof an activity, quantity, or number of extracellular components producedby, excreted by, or associated with a cell.

In this embodiment, heat can be generated in the target structure fromthe light from the at least one upconverter, and the heat can enhancethe induction of the predetermined change. In this embodiment, thepredetermined change can modify the target structure and modulate thebiological activity of the target structure thus treating a condition,disorder or disease affecting the target structure.

In one embodiment, there is provided a system for energy upconversion.The system includes at least one upconverter configured in such a waythat upon exposure to a first set of radiation having a wavelength λ₁ orcentered around wavelength λ₁ (also known as a frequency window centeredaround frequency f1 or ν₁), to generate a second set of radiationcentered around wavelength λ₂ having a higher quantum energy level thanthe first set of radiation centered around or having wavelength λ₁. Therange of frequencies in a frequency window centered on a desirablecenter frequency can be very narrow, and under ideal conditions, thefrequency window contains only one monochromatic radiation having asingle frequency.

In another embodiment, there is provided a system for producing aphotostimulated reaction in a medium. The system includes at least oneupconverter configured, upon exposure to a first radiation havingwavelength λ₁, to generate a second radiation having wavelength λ₂ witha higher quantum energy level than the first radiation having wavelengthλ₁.

Sterilization and Cold Pasteurization of Fluids

Table 1 included below shows appropriate intensities for germicidaldestruction with UV light irradiation.

TABLE 1 Germicidal energies needed to destroy Approximate intensity(μW/cm²) required for 99% destruction of microorganisms: Bacteria  10400 Protozoa (single celled organism) 105 000 Paramecium (slipper shapedprotozoa) 200 000 Chlorella (unicellular fresh-water alga)  13 000Flagellate(protozoan or alga with flagella)  22 000 Sporozoan (parasiticprotozoans) 100 000 Virus  8 000

In this application, it is known that ultraviolet (UV) with a wavelengthof 254 nm tends to inactivate most types of microorganisms. Most juicesare opaque to UV due to the high-suspended solids in them and hence theconventional UV treatment, usually used for water treatment, cannot beused for treating juices. In order to make the process efficient, a thinfilm reactor constructed from glass has been used with the juice flowingalong the inner surface of a vertical glass tube as a thin film. See“Ultraviolet Treatment of Orange Juice” by Tran et al. published inInnovative Food Science & Emerging Technologies (Volume 5, Issue 4,December 2004, Pages 495-502), the entire contents of which areincorporated herein by reference. Tran et al. reported that decimalreduction doses required for the reconstitute orange juices (O J; 10.5°Brix) were 87±7 and 119±17 mJ/cm² for the standard aerobic plate count(APC) and yeast and moulds, respectively. They also reported that theshelf life of fresh squeezed orange juice was extended to 5 days with alimited exposure of UV (73.8 mJ/cm²). The effect of UV on theconcentration of Vitamin C was investigated using both HPLC andtitration methods of measurements. The degradation of Vitamin C was 17%under high UV exposure of 100 mJ/cm², which was similar to that usuallyfound in thermal sterilization. Enzyme pectin methylesterase (PME)activity, which is the major cause of cloud loss of juices, was alsomeasured. The energy required for UV treatment of orange juice (2.0 kWh/m³) was much smaller than that required in thermal treatment (82 kWh/m³). The color and pH of the juice were not significantly influencedby the treatment.

The invention described herein offers advantages over this approach inthat the up converters of the invention can be placed inside fixturessuch as quartz or glass (encapsulation structures) within the orangejuice (or other fluid medium) and irradiated with microwave or RF powersupplied to activate the encapsulated upconverter structures of theinvention in the orange juice.

While discussed with regard to orange juice, any other medium to besterilized including food products, medical products and cosmeticproducts could be treated using the technique of the invention describedherein.

Sterilization of Blood Products

U.S. Pat. No. 6,087,141 (the entire contents of which are incorporatedherein by reference) describes an ultraviolet light activated psoralenprocess for sterilization of blood transfusion products. The inventioncan be applied for the neutralization of AIDS and HIV or other viral orpathogenic agents in blood transfusion products. In this embodiment, atleast one photoactivatable agent is selected from psoralens, pyrenecholesteryloleate, acridine, porphyrin, fluorescein, rhodamine,16-diazorcortisone, ethidium, transition metal complexes of bleomycin,transition metal complexes of deglycobleomycin organoplatinum complexes,alloxazines, vitamin Ks, vitamin L, vitamin metabolites, vitaminprecursors, naphthoquinones, naphthalenes, naphthols and derivativesthereof having planar molecular conformations, porphorinporphyrins, dyesand phenothiazine derivatives, coumarins, quinolones, quinones,anthroquinones, porphycene, rubyrin, rosarin, hexaphyrin, sapphyrin,chlorophyl, chlorin, phthalocynine, porphyrazine, bacteriochlorophyl,pheophytin, texaphyrin macrocyclic-based component, or a metalatedderivative thereof. These photoactivatable agents serve as recipientsfor the secondarily generated light induced by the down conversion orupconversion.

The recipient in this and other embodiments of the invention can includeat least one of a laser dye, a fluorophore, a lumophore, or a phosphor.The laser dye can be at least one of p-terphenyl, sulforhodamine B,p-quaterphenyl, Rhodamine 101, curbostyryl 124, cresyl violetperchlorate, popop, DODC iodide, coumarin 120, sulforhodamine 101,coumarin 2, oxozine 4 perchlorate, coumarin 339, PCM, coumarin 1,oxazine 170 perchlorate, coumarin 138, nile blue A perchlorate, coumarin106, oxatine 1 perchlorate, coumarin 102, pyridine 1, coumarin 314T,styryl 7, coumarin 338, HIDC iodide, coumarin 151, PTPC iodide, coumarin4, cryptocyanine, coumarin 314, DOTC iodide, coumarin 30, HITC iodide,coumarin 500, HITC perchlorate, coumarin 307, PTTC iodide, coumarin 334,DTTC perchlorate, coumarin 7, IR-144, coumarin 343, HDITC perchlorate,coumarin 337, IR-NO, coumarin 6, IR-132, coumarin 152, IR-125, coumarin153, boron-dipyrromethere, HPTS, flourescein, rhodamine 110, 2,7-dichlorofluorescein, rhodamine 65, and rhodamin 19 perchlorate,rhodamine b, and derivatives of these laser dyes that are modified byaddition the addition of appropriate substituents to modify solubilityor tune their interactions within the biological milieu.

In various embodiments of the invention, the recipients are secondaryagents performing other functions. Suitable secondary agents for theinvention include secondary emitters, cytotoxic agents, magneticresonance imaging (MRI) agents, positron emission tomography (PET)agents, radiological imaging agents, or photodynamic therapy (PDT)agents.

These photoactivatable agents (recipients and secondary agents) areintroduced into the blood product (or a patient's blood stream).Microwave or RF power is applied to the blood product (or to thepatient). The gas containing up converter structures of the invention(either included in the blood product) or in encapsulated structuresgenerate secondary light such as UV light which activates thephotoactivatable agents in the blood products. In one embodiment, thegas containing up converter structures of the invention are complexedwith the X-ray down converting particles or other energy modulationagents permitting for example X-ray irradiation to also assist in thisprocess.

In a specific example, the photoactivatable agent is a psoralen, acoumarin, or a derivative thereof, and as discussed above, one cansterilize blood products in vivo (i.e., in a patient) or in a containerof the blood product (such as for example donated blood). The treatmentcan be applied to treat disorders such as for example a cancer cell, atumor cell, an autoimmune deficiency symptom virus, or a blood-bornegermicide is treated by the psoralen, the coumarin, or the derivativethereof.

Waste Water Detoxification

Photocatalysis has also been used as tertiary treatment for wastewaterto comply with regulatory discharge limits and to oxidize compounds thathave not been oxidized in the biological treatment. Photocatalysis hasbeen used to reduce or eliminate several pollutants (e.g., alkanes,alkenes, phenols, aromatics, pesticides) with great success. In manycases, total mineralization of the organic compounds has been observed.Several photocatalysts, such as CdS, Fe₂O₃, ZnO, WO₃, and ZnS, have beenstudied, but the best results have been achieved with TiO₂ P₂₅. Thesephotocatalyst can be used in the invention.

The wastewaters of an oil refinery are the waters resulting from washingthe equipment used in the process, undesirable wastes, and sanitarysewage. These effluents have high oil and grease contents, besides otherorganic compounds in solution. These pollutants form a residual chemicaloxygen demand (COD) that may pose serious toxic hazards to theenvironment.

It is known that photocatalysis can be used for waste water reductionremediation. U.S. Pat. No. 5,118,422 (the entire contents of which areincorporated herein by reference) to Cooper et al. describe anultraviolet driven photocatalytic post-treatment technique for purifyinga water feedstock containing an oxidizable contaminant compound. In thiswork, the water feedstock was mixed with photocatalytic semiconductorparticles (e.g., TiO₂, ZnO, CdS, CdSe, SnO₂, SrTiO₃, WO₃, Fe₂O₃, andTa₂O₅ particles) having a particle size in the range of about 0.01 toabout 1.0 micron and in an amount of between about 0.01% and about 0.2%by weight of the water. The water including the semiconductor mixture isexposed to band-gap photons for a time sufficient to affect an oxidationof the oxidizable contaminant to purify the water. Crossflow membranefiltration was used to separate the purified water from thesemiconductor particles. Cooper et al. show that the organic impuritycarbon content of simulated reclamation waters at nominal 40 PPM levelwere reduced to parts per billion using a recirculation batch reactor.

Cooper et al. identified that one important aspect of the photocatalyticprocess is the adsorption of the organic molecules onto the extremelylarge surface area presented by the finely divided powders dispersed inthe water. Cooper et al. further indicated that, in photoelectrochemicalapplications, advantage is taken of the fact that the solid phase (ametal oxide semiconductor) is also photo-active and that the generatedcharge carriers are directly involved in the organic oxidation. Theadsorption of the band-gap photon by the semiconductor particle resultsin the formation of an electron (e⁻)/hole(h⁺) pair. Cooper et al.explain that the electrons generated in the conduction band react withsolution oxygen forming the dioxygen anion (O₂) species whichsubsequently undergo further reactions resulting in the production ofthe powerfully oxidizing hydroxyl radical species, OH. These powerfuloxidants are known to oxidize organic compounds by themselves.Additionally, Cooper et al. explain that the strongly oxidizing holesgenerated in the valence band have sufficient energy to oxidize allorganic bonds.

In the reactor of Cooper et al., turbulence is necessary in order toensure that the waste water contaminants and the photocatalytic titaniaparticles are exposed to the UV light. Cooper et al. explain that themost basic considerations of photocatalyst light adsorption and itsrelationship to convective mixing. For a 0.1 wt % photocatalyst loading,experiments have shown that 90% of the light is absorbed within 0.08 cm.This is primarily due to the large UV absorption coefficient of thephotocatalyst and therefore, most of the photoelectrochemistry occurswithin this illuminated region. By operating the reactor of Cooper etal. with a Reynolds number (Re) of 4000, a significant portion of thephotoactive region is ensured of being within the well mixed turbulentzone.

Santos et al. have reported in “Photocatalysis as a tertiary treatmentfor petroleum refinery wastewaters” published in Braz. J. Chem. Eng.vol. 23, No. 4, 2006 (the entire contents of which are incorporatedherein by reference), photocatalysis for tertiary treatment forpetroleum refinery wastewaters which satisfactorily reduced the amountof pollutants to the level of the regulatory discharge limits andoxidized persistent compounds that had not been oxidized in thebiological treatment. The treatment sequence used by the refinery(REDUC/PETROBRAS, a Brazilian oil refinery) is oil/water separationfollowed by a biological treatment. Although the process efficiency interms of biological oxygen demand (BOD) removal is high, a residual andpersistent COD and a phenol content remains. The refining capacity ofthe refinery is 41,000 m³/day, generating 1,100 m³/h of wastewater,which are discharged directly into the Guanabara Bay (Rio de Janeiro).Treating the residual and persistent COD remains a priority.

Santos et al. conducted a first set of experiments carried out in anopen 250 mL reactor containing 60 mL of wastewater. In the second set ofexperiments, a Pyrex® annular reactor containing 550 mL of wastewaterwas used (De Paoli and Rodrigues, 1978). The reaction mixtures insidethe reactors were maintained in suspension by magnetic stirring. In allexperiments, air was continuously bubbled through the suspensions. A 250W Phillips HPL-N medium pressure mercury vapor lamp (with its outer bulbremoved) was used as the UV-light source (radiant flux of 108 J·m⁻²·s⁻¹at 8>254 nm). In one set of experiments, the lamp was positioned abovethe surface of the liquid at a fixed height (12 cm). In the second set,the lamp was inserted into the well. All experiments by Santos et al.were performed at 25±1° C. The catalyst concentration ranged from 0.5 to5.5 g L⁻¹ and the initial pH ranged from 3.5 to 9.

In one embodiment of the invention described herein, the up convertersof the invention would be placed inside quartz or glass fixtures withinthe waste water or would be placed on silica encapsulated structureswithin the waste water which, like the photocatalytic TiO₂, could beentrained in the waste water during the irradiation.

Upon irradiation with for example microwave or RF power activation ofthe gas containing upconverter structures of the invention wouldgenerate UV light in nearby presence of the photocatalytic agent. Inother words for this embodiment, the gas containing upconverterstructures of the invention are mixed along with the photocatalyticsemiconductor particles in the waste water fluid stream, and theexterior activation energy source penetrates the container (e.g., aplastic or aluminum container) and irradiates the bulk of the wastewater, producing UV light throughout the waste water which in turndrives the photocatalytic reactions. In one embodiment, the upconvertersof the invention are complexed with the X-ray down converting particlesor other energy modulation agents permitting for example X-rayirradiation to also assist in this process.

In other embodiment, light from the gas containing upconverterstructures would be used in conjunction with more conventional microwavechemical processing to facilitate the chemical processing. U.S. Pat.Nos. 4,946,797 and 5,840,583 (both of which are incorporated herein byreference)

U.S. Pat. No. 4,946,797 describes a process where microwave energy isapplied to an acid/sample mixture at the beginning of, and thereafterduring protein digestion. After the application of microwave energy isdiscontinued, the digestate is diluted by pulsed addition of water,followed by continuous addition of water. Dilution in this mannerprevents a sudden surge in gas evolution, and eliminates the need for anintervening cooling step, thereby reducing processing time. In thepresent invention, the application of light from the gas containingupconverter structures of the invention, especially in the UV wavelengthrange would facilitate in the digestion of these mixtures eitherdirectly or through the use of the catalyst as described above.

U.S. Pat. No. 5,840,583 describes a method for microwave assistedchemical processes that comprises applying sufficient microwaveradiation to a temperature-monitored mixture of reagents, with at leastone of the reagents being thermally responsive to electromagneticradiation in the microwave range, and based on the monitoredtemperature, to maintain the added reagents at or closely about apredetermined temperature while substantially avoiding thermal dilution(or before substantial thermal dilution can occur) that otherwise wouldhave been caused by the addition of the reagents to one another. The'583 patent describes that treatments usually represent oxidation ofsamples and thus include conversion of carbon to carbon dioxide andhydrogen to water or water vapor. Some of the oxidation procedures thatuse liquid oxidizing agents such as the mineral acids are referred to as“wet ashing,” “wet-oxidation,” or “digestion.” In the present invention,the application of light from the gas containing upconverter structuresof the invention, can further assist the thermally responsive agents(the liquid oxidizing agents) in the digestion of these mixtures eitherdirectly or through the use of the catalyst as described above.

Photostimulation

Photostimulation is a field in which light is applied to in order toalter or change a physical property. For example, there has been anincreased focus on the use of biodegradable polymers in consumer andbiomedical fields. Polylactic acid (PLA) plastics andpolyhydroxyalkanoates (PHA) plastics have been playing a vital role infulfilling the objectives. But their relatively hydrophobic surfaceslimit their use in various applications. Hence, there is a need tosurface modify these film surfaces. Due to the lack of any modifiableside chain groups, workers have used a sequential two step photograftingtechnique for the surface modification of these biopolymers. In stepone, benzophenone was photografted on the film surface and in step two,hydrophilic monomers like acrylic acid and acrylamide werephotopolymerized from the film surfaces.

Workers have found that UV irradiation could realize an effective graftcopolymerization. UV-assisted photografting in ethanol has been used togrow hydrophilic polymers (e.g., poly(acrylic acid) and polyacrylamide)from the surfaces of PLA, PHA, and PLA/PHA blend films. In that work, afunctional polyurethane (PU) surface was prepared by photo-graftingN,N-dimethylaminoethyl methacrylate (DMAEM) onto the membrane surface.Grafting copolymerization was conducted by the combined use of thephoto-oxidation and irradiation grafting. PU membrane was photo-oxidizedto introduce the hydroperoxide groups onto the surface, then themembrane previously immersed in monomer solution was irradiated by UVlight. Results have shown prior to the invention that UV irradiation canrealize graft copolymerization effectively.

In the invention described herein, these processes are expedited by theinclusion of the upconverter structures of the invention in dispersionin the fluid medium being used for photostimulation. Upon microwave orRF power irradiation, the upconverters of the invention would generateUV light permitting batch or bulk type processing to occur in parallelinside the container.

Photodeactivation

In many industrial processes, especially food and beverage industries,yeasts are used to produce changes in a medium such as the conversion ofsugars in the raw product. One particularly prominent example is in thewine industry. Stopping the wine from fermenting any further wouldpreserve the current level of sweetness. Likewise, allowing the wine tocontinue fermenting further would only make the wine less sweet witheach passing day. Eventually the wine would become completely dry atwhich time the fermentation would stop on its own. This is becauseduring the fermentation process yeast turns the sugar into alcohol.

Wanting to stop the fermentation process is all good in and of itself.But unfortunately, there is really no practical way to successfully stopa fermentation dead in its tracks. Additives such as sulphite andsorbate can be added to stabilize a fermented product and stopadditional fermentation. Many winemakers will turn to sulfites such asthat found in Sodium Bisulfite or Campden tablets for the answer. But,these two items are not capable of reliably killing enough of the yeastto guarantee a complete stop of the activity—at least not at normaldoses that leave the wine still drinkable.

Once the bulk of the sulfites from either of these ingredients dissipatefrom the wine into the air—as sulfites do—there is a very strong chancethat the remaining few live yeast cells will start multiplying andfermenting again if given enough time. This usually happens at a mostinconvenient time, like after the wine has been bottled and stowed away.

Potassium sorbate is another ingredient that many winemakers considerwhen trying to stop a wine from fermenting any further. There is a lotof misunderstanding surrounding this product. It is typically called forby home wine making books when sweetening a wine. This is a situationwhere the fermentation has already completed and is ready for bottling.One adds the potassium sorbate along with the sugar that is added forsweetening.

The potassium sorbate stops the yeast from fermenting the newly addedsugar. So, many winemakers assume potassium sorbate can stop an activefermentation as well, but, potassium sorbate does not kill the yeast atall, but rather it makes the yeast sterile. In other words, it impairsthe yeast's ability to reproduce itself. But, it does not hinder theyeast's ability to ferment sugar into alcohol.

Ultraviolet light is known to destroy yeast cultures, but has restrictedapplications due to the inability of UV light to penetrate throughoutthe fluid medium. While heat can be used to destroy the yeast activity,cooking of the product may be premature or may produce undesirablechanges in the consistency and taste. For liquid or fluid food products,the same techniques described above could be used for the applicationdescribed here. For non-liquid products, energy modulation agents withlittle and preferably no toxicity (e.g. Fe oxides or titanium oxides)could be added. Here, the concentration of these additives would likelybe limited by any unexpected changes in taste.

Here, UV light produced by the up converters of the invention woulddeactivate the yeasts.

Photoactivated Cross-Linking and Curing of Polymers

In this application, the upconverters of the invention are provided anddistributed into an uncured polymer based medium for the activation ofphotosensitive agents in the medium to promote cross-linking and curingof the polymer based medium. In one embodiment, the upconverters of theinvention are complexed with other down-converting luminescent particlesor other energy modulation agents prior to being added to the polymer.

For adhesive and surface coating applications, light activatedprocessing is limited due to the penetration depth of UV light into theprocessed medium. In light activated adhesive and surface coatingprocessing, the primary limitation is that the material to be cured mustsee the light—both in type (wavelength or spectral distribution) andintensity. This limitation has meant that one medium typically has totransmit the appropriate light. In adhesive and surface coatingapplications, any “shaded” area will require a secondary cure mechanism,increasing cure time over the non-shaded areas and further delaying curetime due to the existent of a sealed skin through which subsequentcuring must proceed.

Conventionally, moisture-curing mechanisms, heat-curing mechanisms, andphoto-initiated curing mechanisms are used to initiate cure, i.e.,cross-linking, of reactive compositions, such as reactive silicones,polymers, and adhesives. These mechanisms are based on eithercondensation reactions, whereby moisture hydrolyzes certain groups, oraddition reactions that can be initiated by a form of energy, such aselectromagnetic radiation or heat.

The invention described herein can use any of the following lightactivated curing polymers as well as others known in the art to whichthe upconverters of the invention are added.

For example, one suitable light activated polymer compound includes UVcuring silicones having methacrylate functional groups. U.S. Pat. No.4,675,346 to Lin, the disclosure of which is hereby expresslyincorporated herein by reference, is directed to UV curable siliconecompositions including at least 50% of a specific type of siliconeresin, at least 10% of a fumed silica filler and a photoinitiator, andcured compositions thereof. Other known UV curing silicone compositionssuitable for the invention include organopolysiloxane containing a(meth)acrylate functional group, a photosensitizer, and a solvent, whichcures to a hard film. Other known UV curing silicone compositionssuitable for the invention include compositions of an organopolysiloxanehaving an average of at least one acryloxy and/or methacryloxy group permolecule; a low molecular weight polyacrylyl crosslinking agent; and aphotosensitizer.

Loctite Corporation has designed and developed UV and UV/moisture dualcurable silicone compositions, which also demonstrate high resistance toflammability and combustibility, where the flame-retardant component isa combination of hydrated alumina and a member selected from the groupconsisting of organo ligand complexes of transition metals,organosiloxane ligand complexes of transition metals, and combinationsthereof. See U.S. Pat. Nos. 6,281,261 and 6,323,253 to Bennington. Theseformulations are also suitable for the invention.

Other known UV photoactivatable silicones include siliconesfunctionalized with, for example, carboxylate, maleate, cinnamate andcombinations thereof. These formulations are also suitable for theinvention. Other known UV photoactivatable silicones suitable for theinvention include benzoin ethers (“UV free radical generator”) and afree-radical polymerizable functional silicone polymers, as described inU.S. Pat. No. 6,051,625 whose content is incorporated herein byreference in its entirety. The UV free radical generator (i.e., thebenzoin ether) is contained at from 0.001 to 10 wt % based on the totalweight of the curable composition. Free radicals produced by irradiatingthe composition function as initiators of the polymerization reaction,and the free radical generator can be added in a catalytic quantityrelative to the polymerizable functionality in the subject composition.

Further included in these silione resins can be silicon-bonded divalentoxygen atom compounds which can form a siloxane bond while the remainingoxygen in each case can be bonded to another silicon to form a siloxanebond, or can be bonded to methyl or ethyl to form an alkoxy group, orcan be bonded to hydrogen to form silanol. Such compounds can includetrimethylsilyl, dimethylsilyl, phenyldimethylsilyl, vinyldimethylsilyl,trifluoropropyldimethylsilyl, (4-vinylphenyl)dimethylsilyl,(vinylbenzyl)dimethylsilyl, and (vinylphenethyl)dimethylsilyl.

The photoinitiator component of the invention is not limited to thosefree radical generators given above, but may be any photoinitiator knownin the art, including the afore-mentioned benzoin and substitutedbenzoins (such as alkyl ester substituted benzoins), Michler's ketone,dialkoxyacetophenones, such as diethoxyacetophenone (“DEAP”),benzophenone and substituted benzophenones, acetophenone and substitutedacetophenones, and xanthone and substituted xanthones. Other desirablephotoinitiators include DEAP, benzoin methyl ether, benzoin ethyl ether,benzoin isopropyl ether, diethoxyxanthone, chloro-thio-xanthone,azo-bisisobutyronitrile, N-methyl diethanolaminebenzophenone, andmixtures thereof. Visible light initiators include camphoquinone,peroxyester initiators and non-fluorene-carboxylic acid peroxyesters.

Commercially available examples of photoinitiators suitable for theinvention include those from Vantico, Inc., Brewster, N.Y. under theIRGACURE and DAROCUR tradenames, specifically IRGACURE 184(1-hydroxycyclohexyl phenyl ketone), 907(2-methyl-1-[4-(methylthio)phenyl]-2-morpholino propan-1-one), 369(2-benzyl-2-N,N-dimethylamino-1-(4-morpholinophenyl)-1-butanone), 500(the combination of 1-hydroxy cyclohexyl phenyl ketone andbenzophenone), 651 (2,2-dimethoxy-2-phenyl acetophenone), 1700 (thecombination of bis(2,6-dimethoxybenzoyl-2,4,4-trimethyl pentyl)phosphine oxide and 2-hydroxy-2-methyl-1-phenyl-propan-1-one), and 819[bis(2,4,6-trimethyl benzoyl)phenyl phosphine oxide] and DAROCUR 1173(2-hydroxy-2-methyl-1-phenyl-1-propane) and 4265 (the combination of2,4,6-trimethylbenzoyldiphenyl-phosphine oxide and2-hydroxy-2-methyl-1-phenyl-propan-1-one); and IRGACURE 784DC(bis(.eta.sup.5-2,4-cyclopentadien-1-yl)-bis[2,6-difluoro-3-(1H-pyrrol-1-yl)phenyl]titanium).

Generally, the amount of photoinitiator (or free radical generators)should be in the range of about 0.1% to about 10% by weight, such asabout 2 to about 6% by weight. The free radical generator concentrationfor benzoin ether is generally from 0.01 to 5% based on the total weightof the curable composition.

A moisture cure catalyst can also be included in an amount effective tocure the composition. For example, from about 0.1 to about 5% by weight,such as about 0.25 to about 2.5% by weight, of the moisture curecatalyst can be used in the invention to facilitate the cure processbeyond that of photo-activated curing. Examples of such catalystsinclude organic compounds of titanium, tin, zirconium and combinationsthereof. Tetraisopropoxytitanate and tetrabutoxytitanate are suitable asmoisture cure catalyst. See also U.S. Pat. No. 4,111,890, the disclosureof which is expressly incorporated herein by reference.

Included in the conventional silicone composition (and other inorganicand organic adhesive polymers) suitable for the invention are variousinorganic fillers. For example, hollow microspheres supplied by Kishunder the trade name Q-CEL are free flowing powders, white in color.Generally, these borosilicate hollow microspheres are promoted asextenders in reactive resin systems, ordinarily to replace heavyfillers, such as calcium carbonate, thereby lowering the weight ofcomposite materials formed therewith. Q-CEL 5019 hollow microspheres areconstructed of a borosilicate, with a liquid displacement density of0.19 g/cm², a mean particle size of 70 microns, and a particle sizerange of 10-150 um. Other Q-CEL products are shown below in tabularform. Another commercially available hollow glass microsphere is sold byKish under the trade name SPHERICEL. SPHEREICEL 110P8 has a meanparticle size of about 11.7 microns, and a crush strength of greaterthan 10,000 psi. Yet other commercially available hollow glassmicrosphere are sold by the Schundler Company, Metuchen, N.J. under thePERLITE tradename, Whitehouse Scientific Ltd., Chester, UK and 3M,Minneapolis, Minn. under the SCOTCHLITE tradename.

In general, these inorganic filler components (and others such as fumedsilica) add structural properties to the cured composition, as well asconfers flowability properties to the composition in the uncured stateand increase the transmissivity for the UV cure radiation. When present,the fumed silica can be used at a level of up to about 50 weightpercent, with a range of about 4 to at least about 10 weight percent,being desirable. While the precise level of silica may vary depending onthe characteristics of the particular silica and the desired propertiesof the composition and the reaction product thereof, care should beexercised by those persons of ordinary skill in the art to allow for anappropriate level of transmissivity of the inventive compositions topermit a UV cure to occur.

Desirable hydrophobic silicas include hexamethyldisilazane-treatedsilicas, such as those commercially available from Wacker-Chemie,Adrian, Mich. under the trade designation HDK-2000. Others includepolydimethylsiloxane-treated silicas, such as those commerciallyavailable from Cabot Corporation under the trade designation CAB-O-SILN70-TS, or Degussa Corporation under the trade designation AEROSIL R202.Still other silicas include trialkoxyalkyl silane-treated silicas, suchas the trimethoxyoctyl silane-treated silica commercially available fromDegussa under the trade designation AEROSIL R805; and 3-dimethyldichlorosilane-treated silicas commercially available from Degussa underthe trade designation R972, R974 and R976.

While these inorganic fillers have extended the use of conventional UVcured silicone systems to permit the curing of materials beyond a skindepth of UV penetration, these inorganic fillers alone do not overcomeshadowing effects and suffer from UV scattering which effectively makesfor a smaller penetration depth. In the invention described herein, theinclusion of these inorganic fillers along with luminescent particlesprovide a mechanism by which uniform light activated cures can occurdeep inside of the body of adhesive-solidified assemblies in regionsthat would normally be shadowed or not with the reach of external UV orother light sources.

Accordingly, in this example of the invention described herein,conventional silicone and polymeric adhesive or release or coatingcompositions are prepared using conventional mixing, heating, andincubation techniques. Included in these conventional compositions arethe upconverter structures of the invention. These compositions can thenbe applied to surfaces of objects to be fixed together or to surfaceswhere a hard coating is desired or cast in a curable form for theproduction of molded objects. These compositions upon activation willproduce radiant light for photoactivated cure of the luminescentparticle containing polymer composition. The density of the upconverterstructures in these compositions will depend on the “light transparency”of the luminescent particle containing composition. Where thesecompositions contain a significant amount of the inorganic filler asdiscussed above, the concentration of the upconverter structures can bereduced for example as compared to a composition with a black colorpigment where the light transparency will be significantly reduced.

U.S. Pat. No. 7,294,656 to Bach et al., the entire disclosure of whichis incorporated herein by reference, describes a non-aqueous compositioncurable by UV radiation broadly containing a mixture of two UV curableurethane acrylates that have several advantages over conventionalradiation-curable compositions. The Bache et al. compositions can becured in a relatively short time using UV-C (200-280 nm), UV-B (280-320nm), UV-A (320-400 nm) and visible (400 nm and above) radiation. Inparticular, Bache et al. compositions can be cured using radiationhaving a wavelength of 320 nm or more. When fully cured (regardless ofthe type of radiation used), the Bach et al. compositions exhibithardnesses and impact resistances at least comparable to conventionalcoatings.

In the invention described here, the upconverters are added to theseBach et al. compositions. Due to the fact that the exterior energysource penetrates deeper into the entirety of the Bach et al.compositions, thicker surface coatings can be realized. Further, thecoatings can be applied to intricate surfaces having for example beenprepared with recesses or protrusions.

Electromagnetic Field Visualization Probe

The gas containing up converter structures of the invention in oneembodiment are designed to produce plasma ignition under low Q, lowfield conditions such that inadvertent heating does not occur in themedium where the upconverters are dispersed. This capability permitsthen the upconverters of the invention to be used in encapsulations onor near (or removable and insertable) high power electromagneticsources. For example, in the testing and development of microwavecircuitry, one often has to infer as to the paths of microwave leakage(especially if the paths of microwave leakage or operating at harmonicfrequencies). In on embodiment, isolated gas cavities filled withioniozable gas can be packing for example in a wand made of anelectrically insulating material to protect the user. The wand wouldthen be used as a test probe to probe regions of high electric fieldstrength. Alternatively, in one embodiment, the wand would include amicrowave antenna connected to a microwave power supply. The fieldstrength from the antenna would not normally (in absence of an externalfield) produce plasma ignitions in the isolated gas cavities.

At low powers, the wand could physically probe the microwave fieldstrength with areas of high field strength producing plasma ignition andoptical emission from the wand which would be visible to the user. Thesmall size of the cavities in the broad band upconverters of theinvention would be advantageous for not drawing significant power fromthe microwave circuit being evaluated.

In another embodiment, the wand could be designed for the testing ofhigh power AC and RF circuits or transformers. In this embodiment, thewand could also include the afore-mentioned microwave antenna providinga local source of microwave power to the isolated gas cavities. Thepower level would be set below an ignition threshold of the gas cavity.However, as the wand and the isolated gas cavities were moved into aregion of high electric field, the high electric field would supplementenergy from the microwave antenna and produce plasma ignitions.

In another embodiment, the wand would include isolated gas cavitieswhere different ones of the gas cavities would be filled with gases ofdifferent ionization potentials or at different pressures. The gasesigniting first would have one color, while gases igniting later athigher potentials would show a different color. In this way, a relativemagnitude of the electric field would be manifest by the differentcolors. For example, blue emission could be established with argon, anda red emission could be established with nitrogen such that the bluewould be regarded by the user to the representative of a relatively lowelectric field strength and the red emission would be representative ofa relatively higher electric field strength.

In some environments, workers for example on high power, high tensionelectrical lines would use the wands as safety checks on the presence ofpower. In this aspect, no contact of the wand to the high tension deviceis required to ascertain the presence of power on the lines.

Light Sources

The gas containing up converter structures of the invention in oneembodiment are designed to produce plasma ignition under low Q, lowfield conditions such that inadvertent heating does not occur in themedium where the upconverters are dispersed. This capability permitsthen the upconverters of the invention to be used as light sourcessimilar to the microcavity light sources described above. Themicrocavity light sources described above depend on capacitive electricfield coupling to generate the plasma responsible for light emission.This power coupling mechanism inherently heats the anode of the lightingdevice, ultimately limiting power to a point where local heatingdestroys the material of the microcavity light source. Conversely, thispower coupling mechanism requires a high value of electric fieldstrength and voltage to sustain a plasma. Indeed, the microcavity lightsources described above typically requires 100's of volts for plasmaoperation.

Microwave coupling avoids these issues and is an electrodeless way tocouple power without then the anode loss problem.

Inspection Probes

As noted above, microwave coupling avoids these issues and is anelectrodeless way to couple power without then the anode loss problem.While this may permit higher luminance from microcavity devices to beobtained, it may also permit lower powers to be used to obtain emission.

Because of the sensitivity of the human eye and modern detectors, evenlow level luminoscity devices can be of utility in diagnostic areas. Forexample, in the inspection of many macroscopic construction articles,(such as for example steel structures, metal castings, concretepourings, plastic moldings, asphalt pavings, etc.), the human eye andstaining techniques are typically used. Beyond that, more expensivex-ray and ultrasound techniques are used.

Here, the gas containing up converter structures of the invention in oneembodiment are of a microscopic size such that the upconverters could beapplied to the surface of an article of manufacture. For example, theupconverters could be suspended in a solution and washed over the pieceto be tested for cracks. The microscopic size would mean that the broadband upconverters would preferentially be retained in the non-surfaceareas (e.g., in the cracks or pits of the concrete). Irradiation with ahand held microwave source (or placement of the piece inside a microwaveresonator) would produce plasma emission whose intensity would show morestrongly where more of the upconverters had settled. Digital camerascould then be used to document where the defects occurred.

Having generally described this invention, a further understanding canbe obtained by reference to certain specific examples which are providedherein for purposes of illustration only and are not intended to belimiting unless otherwise specified.

Numerous modifications and variations of the invention are possible inlight of the above teachings. It is therefore to be understood thatwithin the scope of the appended claims, the invention may be practicedotherwise than as specifically described herein.

The invention claimed is:
 1. A system for generating light, comprising:a low frequency energy source which radiates a first wavelength λ₁ ofradiation; and a free-standing receptor having outside dimensions ofmillimeters or below and which receives the first wavelength λ₁ ofradiation and generates a second wavelength λ₂ of the emitted light inthe infrared visible or the ultraviolet wavelength range; wherein thefree-standing receptor comprises: a partitioned structure including atleast two reaction components; and a partition separating the at leasttwo reaction components whereby mixing of the two reaction componentsupon microwave radiation at first wavelength λ₁ produces at least one ofa chemiluminescent or bioluminescent reaction for emission of the secondwavelength λ₂.
 2. The system of claim 1, wherein the receptor comprisesan ionizable-gas containment sealed with an ionizable gas and includinga free space region within the containment, which upon ionization emitsat least the second wavelength λ₂.
 3. The system of claim 2, wherein theionizable-gas containment has an outside dimension less than 10 mm. 4.The system of claim 2, wherein the ionizable gas containment has anoutside dimension less than 1000 nm.
 5. The system of claim 2, whereinthe ionizable-gas containment has an outside dimension less than 100 nm.6. The system of claim 2, wherein the ionizable-gas containmentcomprises a porous structure permeable to microwave or rf radiation. 7.The system of claim 6, wherein the porous structure comprises at leastone of a silicate glass, an alkali glass, a sodium glass, and aphosphate glass.
 8. The system of claim 6, wherein the porous structurecomprises an ion-exchanged glass structure.
 9. The system of claim 6,wherein the porous structure comprises an outside water glass to sealsaid ionizable gas inside.
 10. The system of claim 2, wherein theionizable-gas containment comprises at least one of a silica gel, aprecipitate silicate, a cenosphere, a conductosphere, or a hollowsphere.
 11. The system of claim 2, wherein the ionizable-gas containmentcomprises at least one of hydrogen, argon, nitrogen, xenon, ammonia,iodine vapor; mercury vapor; an organic gas, and hydrogen-nitrogenmixtures, and mixtures thereof.
 12. The system of claim 2, wherein theionizable-gas containment comprises a microwave or rf coupler to promoteelectron emission into the free space region.
 13. The system of claim 2,wherein the microwave or rf coupler comprises at least one of a carbonstructure, a carbon nanotube, a single wall carbon nanotube, a doublewall carbon nanotube, grapheme, and metal materials made of aluminum orcopper.
 14. The system of claim 1, wherein the at least two reactioncomponents comprise two bioluminescent reagents.
 15. The system of claim1, wherein the at least two reaction components comprise twochemiluminescent reagents.
 16. The system of claim 1, wherein thepartition comprises a microwave-activatable material which, uponactivation, opens the partition to mix the at least two reactioncomponents.
 17. The system of claim 16, wherein the partition comprisesat least one of a microwave susceptible material which heats uponmicrowave exposure, or a rf susceptible material which heats upon rfexposure, or a magnetic susceptible material which is inductively movedupon exposure to a magnetic inductive field.
 18. The system of claim 16,wherein the partition comprises a melting point material less than 30°C.
 19. The system of claim 1, wherein the partitioned structurecomprises a biodissovable material.
 20. The system of claim 16, whereinthe partition comprises a material having a melting point greater than30° C.
 21. The system of claim 20, wherein the receptor comprises astructure including a shell and at least one interior void.
 22. Thesystem of claim 21, wherein said structure comprises at least one of acenosphere and a conductosphere.
 23. The system of claim 21, whereinsaid interior void is filled with at least one argon, neon, xenon,helium, ammonia, or an organic molecule.
 24. The system of claim 1,further comprising: a microwave or rf applicator which directs saidfirst wavelength λ₁ into an object including said microwave receptor.25. The system of claim 24, wherein the microwave or rf applicatorcomprises one of a waveguide applicator, a microwave or rf antenna, or amicrowave beam source.
 26. The system of claim 25, wherein the microwavebeam source comprises a focused beam source concentration radiation ofsaid first wavelength λ₁ into a region of said object where saidmicrowave receptors reside.
 27. The system of claim 1, wherein saidfirst wavelength λ₁ radiation is in a range of 1 KHz to 100 GHz.
 28. Thesystem of claim 1, wherein the receptor is configured to emit for saidsecond wavelength λ₂ radiation which activates psoralen.
 29. The systemof claim 1, wherein the receptor is configured to emit for said secondwavelength λ₂ radiation which photoactivates a photoinitiator in a resinmaterial.
 30. The system of claim 1, wherein the receptor is configuredto emit for said second wavelength λ₂ radiation which is capable ofsterilizing a medium in vicinity of the microwave receptor.
 31. Thesystem of claim 1, wherein the receptor is configured to emit for saidsecond wavelength λ₂ radiation which photoactivates a photo-activatableadhesive connecting members together.
 32. The system of claim 31,wherein said members comprise at least one of a semiconductor device, aprinted circuit board, or a semiconductor wafer.
 33. The system of claim1, wherein the receptor is configured to emit for said second wavelengthλ₂ radiation which photoactivates photograftable materials.
 34. Thesystem of claim 1, wherein the receptor comprises a plurality ofreceptors forming a fluidized bed for treating a fluid about thereceptors.
 35. The system of claim 1, wherein the receptor is configuredto emit for said second wavelength λ₂ radiation in a range from NIR toUV.
 36. A microwave or rf receptor comprising: a partitioned structureincluding at least two reaction components; and a partition separatingthe at least two reaction components, whereby mixing of the two reactioncomponents upon microwave or rf radiation at first wavelength λ₁produces at least one of a chemiluminescent or bioluminescent reactionfor emission of the second wavelength λ₂.
 37. The receptor of claim 36,wherein the at least two reaction components comprise two bioluminescentreagents.
 38. The receptor of claim 36, wherein the at least tworeaction components comprise two chemiluminescent reagents.
 39. Thereceptor of claim 36, wherein the partition comprises a microwave orrf-activatable material which, upon activation, opens the partition tomix the at least two reaction components.
 40. The receptor of claim 36,wherein the partitioned structure comprises a biodissovable material.41. The receptor of claim 36, wherein the partition comprises a materialhaving a melting point material less than 30° C.
 42. The receptor ofclaim 36, wherein the partitioned structure comprises a biocompatiblematerial.
 43. The receptor of claim 36, wherein the partitionedstructure comprises a material having a melting point greater than 30°C.
 44. The receptor of claim 36, wherein the partitioned structurecomprises a structure including a shell and at least one interior void.45. The receptor of claim 36, wherein said partitioned structurecomprises at least one of a cenosphere and a conductosphere.
 46. Thereceptor of claim 36, wherein said partitioned structure has microscopicdimensions.
 47. A method for generating light using the microwave or rfreceptor of claim 36, comprising: exposing the microwave or rf receptorto the first wavelength λ₁ of radiation; upon interaction of said firstwavelength λ₁ of radiation with the microwave or rf receptor, initiatingmixing of the at least two reaction components to produce therefrom theat least one of the chemiluminescent or the bioluminescent reaction,thus generating the second wavelength λ₂ of radiation in the infrared,visible, or ultraviolet wavelength range.
 48. The method of claim 47,further comprising: mixing two bioluminescent reagents.
 49. The methodof claim 47, further comprising: mixing two chemiluminescent reagents.50. The method of claim 47, further comprising: opening a partitionseparating the at least two reagents upon exposure to said firstwavelength λ₁ of radiation.
 51. The method of claim 50, wherein saidopening comprises: melting said partition or rupturing said partitionwith an applied microwave, radio frequency wave, ultrasound wave, ormagnetic induction field.
 52. The method of claim 47, furthercomprising: directing said first wavelength λ₁ of radiation into anobject including said receptor.
 53. The method of claim 47, furthercomprising: focusing said first wavelength λ₁ of radiation into anobject including said receptor.
 54. The method of claim 47, wherein saidproducing comprises: generating, for said first wavelength λ₁ ofradiation, radiation in a range from 10 MHz to 100 GHz.
 55. The methodof claim 47, further comprising: interacting said second wavelength λ₂of radiation with psoralen.
 56. The method of claim 47, furthercomprising: interacting said second wavelength λ₂ of radiation withphotoactivatable resin to cure said medium.
 57. The method of claim 47,further comprising: interacting said second wavelength λ₂ of radiationwith a medium to sterilize the medium.
 58. The method of claim 47,further comprising: interacting said second wavelength λ₂ of radiationwith a photoactivatable adhesive.
 59. The method of claim 47, furthercomprising: interacting said second wavelength λ₂ of radiation with aphoto-graftable material.
 60. The method of claim 47, wherein saidgenerating comprises: producing, for said second wavelength λ₂ ofradiation, radiation in a range of IR to UV light.
 61. The method ofclaim 47, further comprising: placing two members together with aphoto-activatable medium in between including said receptors;transmitting said first wavelength λ₁ of radiation through at least oneof said two members to interact with said receptors; and binding the twomembers together by interaction of said second wavelength λ₂ ofradiation with the photoactivatable medium.
 62. The method of claim 61,wherein said placing comprises: placing two semiconductor elementstogether, and bonding the two semiconductor elements together.
 63. Themethod of claim 61, wherein said placing comprises: placing two printedcircuit board elements together; and bonding the two printed circuitboard elements together.